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<section id="glossary">
<span id="id1"></span><h1>Glossary<a class="headerlink" href="#glossary" title="Permalink to this heading"></a></h1>
<p>The glossary is partly extracted from New Manual of Observatory Practice and some information
is taken from Modern Global Seismology.</p>
<section id="scname-terms">
<h2><cite>SeisComP</cite> terms<a class="headerlink" href="#scname-terms" title="Permalink to this heading"></a></h2>
<dl class="glossary">
<dt id="term-binding">binding<a class="headerlink" href="#term-binding" title="Permalink to this term"></a></dt><dd><p>A binding is a set of configuration options to configure the connection between a
<a class="reference internal" href="#term-module"><span class="xref std std-term">module</span></a> and a station. Bindings are located in <code class="docutils literal notranslate"><span class="pre">etc/key/modulename/station_NET_STA</span></code>.
They are either written to the database or used to create native configuration files
for standalone modules. The concepts section on <a class="reference internal" href="concepts/configuration.html#concepts-configuration"><span class="std std-ref">configuration</span></a>
provides more details.</p>
</dd>
<dt id="term-module">module<a class="headerlink" href="#term-module" title="Permalink to this term"></a></dt><dd><p>A module is usually a binary executable that does a certain job such as <a class="reference internal" href="../apps/seedlink.html#seedlink"><span class="std std-ref">seedlink</span></a>
or <a class="reference internal" href="../apps/scautopick.html#scautopick"><span class="std std-ref">scautopick</span></a>. The concepts section on <a class="reference internal" href="concepts/modules.html#concepts-modules"><span class="std std-ref">modules</span></a>
provides more details.</p>
</dd>
<dt id="term-plugin">plugin<a class="headerlink" href="#term-plugin" title="Permalink to this term"></a></dt><dd><p>An extension to a module. The concepts section on <a class="reference internal" href="concepts/plugins.html#concepts-plugins"><span class="std std-ref">plugins</span></a>
provides more details.</p>
</dd>
<dt id="term-profile">profile<a class="headerlink" href="#term-profile" title="Permalink to this term"></a></dt><dd><p>A profile is a special <a class="reference internal" href="#term-binding"><span class="xref std std-term">binding</span></a>. Instead of defining the same set of configuration
options again and again for many stations a profile can be used. Instead of configuring a
stations like:</p>
<div class="highlight-sh notranslate"><div class="highlight"><pre><span></span>seedlink
scautopick
</pre></div>
</div>
<p>which refers to <code class="docutils literal notranslate"><span class="pre">etc/key/seedlink/station_NET_STA</span></code> and <code class="docutils literal notranslate"><span class="pre">etc/key/scautopick/station_NET_STA</span></code>
a profile can be given:</p>
<div class="highlight-sh notranslate"><div class="highlight"><pre><span></span>seedlink:geofon
scautopick:teleseismic
</pre></div>
</div>
<p>which refers to <code class="file docutils literal notranslate"><span class="pre">etc/key/seedlink/profile_geofon</span></code> and
<code class="file docutils literal notranslate"><span class="pre">etc/key/scautopick/profile_teleseismic</span></code>.
Changing the profile changes the bindings of all stations that use this profile.</p>
</dd>
<dt id="term-RecordStream">RecordStream<a class="headerlink" href="#term-RecordStream" title="Permalink to this term"></a></dt><dd><p>Interface to access data records from data processing modules.
<a class="reference internal" href="#term-SeisComP"><span class="xref std std-term">SeisComP</span></a> applications access waveform data through the
<a class="reference internal" href="concepts/recordstream.html#concepts-recordstream"><span class="std std-ref">RecordStream interface</span></a>.</p>
</dd>
<dt id="term-standalone-module">standalone module<a class="headerlink" href="#term-standalone-module" title="Permalink to this term"></a></dt><dd><p>A module that needs to convert the configuration or do not use the default
configuration options (see below) is called a standalone modules.
Examples for standalone modules are <a class="reference internal" href="../apps/seedlink.html#seedlink"><span class="std std-ref">seedlink</span></a>, <a class="reference internal" href="../apps/slarchive.html#slarchive"><span class="std std-ref">slarchive</span></a> or <a class="reference internal" href="../apps/slmon.html#slmon"><span class="std std-ref">slmon</span></a>.</p>
</dd>
<dt id="term-trunk">trunk<a class="headerlink" href="#term-trunk" title="Permalink to this term"></a></dt><dd><p>The module and library collection which forms and uses the SeisComP
framework. The Application class is part of this framework. All trunk
modules share a common configuration schema and a database with
Inventory, EventParameters, Configuration, Routing and QC schemas.
Representatives are <a class="reference internal" href="../apps/scautoloc.html#scautoloc"><span class="std std-ref">scautoloc</span></a> and <a class="reference internal" href="../apps/scautopick.html#scautopick"><span class="std std-ref">scautopick</span></a> and the GUI
collection with <a class="reference internal" href="../apps/scolv.html#scolv"><span class="std std-ref">scolv</span></a>, <a class="reference internal" href="../apps/scmv.html#scmv"><span class="std std-ref">scmv</span></a>, <a class="reference internal" href="../apps/scrttv.html#scrttv"><span class="std std-ref">scrttv</span></a> and <a class="reference internal" href="../apps/scesv.html#scesv"><span class="std std-ref">scesv</span></a>.</p>
</dd>
</dl>
</section>
<hr class="docutils" />
<section id="scientific-and-technical-terms">
<h2>Scientific and technical terms<a class="headerlink" href="#scientific-and-technical-terms" title="Permalink to this heading"></a></h2>
<dl class="glossary">
<dt id="term-AIC">AIC<a class="headerlink" href="#term-AIC" title="Permalink to this term"></a></dt><dd><p>Aikaike Information Criterion used for refinement of phase picks.
Phase pickers for picking P and S phase arrivals based on AIC may reach
high accuracy if tuned well.</p>
</dd>
<dt id="term-aftershocks">aftershocks<a class="headerlink" href="#term-aftershocks" title="Permalink to this term"></a></dt><dd><p>Earthquakes that follow a large earthquake in a sequence. They are smaller than the mainshock
and within 1-2 fault lengths distance from the mainshock fault. Aftershocks can continue over
a period of weeks, months, or years, decreasing in frequency with time. In general, the larger
the mainshock, the larger and more numerous the aftershocks, and the longer they will continue.</p>
</dd>
<dt id="term-amplitude">amplitude<a class="headerlink" href="#term-amplitude" title="Permalink to this term"></a></dt><dd><ol class="arabic simple">
<li><p>General term used for an observation of a wave at a particular time.</p></li>
<li><p>QuakeML object. Amplitudes are computed, e.g. for computing
<a class="reference internal" href="#term-magnitude"><span class="xref std std-term">magnitudes</span></a> of different types. Another type is the
<a class="reference internal" href="#term-SNR"><span class="xref std std-term">SNR</span></a>. Amplitude computation depends on the type.</p></li>
</ol>
<p>In <cite>SeisComP</cite> amplitudes are computed automatically by <a class="reference internal" href="../apps/scautopick.html#scautopick"><span class="std std-ref">scautopick</span></a> and
<a class="reference internal" href="../apps/scamp.html#scamp"><span class="std std-ref">scamp</span></a> or interactively by <a class="reference internal" href="../apps/scolv.html#scolv"><span class="std std-ref">scolv</span></a>.</p>
</dd>
<dt id="term-array">array<a class="headerlink" href="#term-array" title="Permalink to this term"></a></dt><dd><p>A set of observing sensors at which the observed and sought signal are mostly coherent.
If the sensors are seismometers or barometers measuring infrasound, the terms
<a class="reference internal" href="#term-seismic-array"><span class="xref std std-term">seismic array</span></a> or <a class="reference internal" href="#term-infrasound-array"><span class="xref std std-term">infrasound array</span></a> are used, respectively.
Arrays are different from a <a class="reference internal" href="#term-network"><span class="xref std std-term">network</span></a> by the applied methods, e.g.
<a class="reference internal" href="#term-F-K"><span class="xref std std-term">F-K</span></a> analysis, <a class="reference internal" href="#term-beam"><span class="xref std std-term">beam</span></a> forming or <a class="reference internal" href="#term-vespagram"><span class="xref std std-term">vespagram</span></a> analysis.</p>
</dd>
<dt id="term-ATF">ATF<a class="headerlink" href="#term-ATF" title="Permalink to this term"></a></dt><dd><p>The <a class="reference internal" href="#term-array-transfer-function"><span class="xref std std-term">array transfer function</span></a> or <a class="reference internal" href="#term-array-response-function"><span class="xref std std-term">array response function</span></a>
describes the sensitivity and resolution of an <a class="reference internal" href="#term-array"><span class="xref std std-term">array</span></a> to signals
propagating through the array with a particular <a class="reference internal" href="#term-azimuth"><span class="xref std std-term">azimuth</span></a>, <a class="reference internal" href="#term-slowness"><span class="xref std std-term">slowness</span></a>
and <a class="reference internal" href="#term-frequency"><span class="xref std std-term">frequency</span></a>.</p>
</dd>
<dt id="term-array-response-function">array response function<a class="headerlink" href="#term-array-response-function" title="Permalink to this term"></a></dt><dd><p>A synonym of <a class="reference internal" href="#term-ATF"><span class="xref std std-term">ATF</span></a> or <a class="reference internal" href="#term-array-transfer-function"><span class="xref std std-term">array transfer function</span></a>.</p>
</dd>
<dt id="term-array-transfer-function">array transfer function<a class="headerlink" href="#term-array-transfer-function" title="Permalink to this term"></a></dt><dd><p>A synonym of <a class="reference internal" href="#term-ATF"><span class="xref std std-term">ATF</span></a> or <a class="reference internal" href="#term-array-response-function"><span class="xref std std-term">array response function</span></a>.</p>
</dd>
<dt id="term-ArcLink">ArcLink<a class="headerlink" href="#term-ArcLink" title="Permalink to this term"></a></dt><dd><p>ArcLink complements <a class="reference internal" href="#term-SeedLink"><span class="xref std std-term">SeedLink</span></a> by providing access to archived waveform
data. Arclink was distributed with <a class="reference internal" href="#term-SeisComP"><span class="xref std std-term">SeisComP</span></a> until version 3.0.</p>
</dd>
<dt id="term-arrival">arrival<a class="headerlink" href="#term-arrival" title="Permalink to this term"></a></dt><dd><ol class="arabic simple">
<li><p>The appearance of seismic energy on a seismic record</p></li>
<li><p>QuakeML object. The detected phase onset associated to an origin in <cite>SeisComP</cite>.</p></li>
</ol>
</dd>
<dt id="term-arrival-time">arrival time<a class="headerlink" href="#term-arrival-time" title="Permalink to this term"></a></dt><dd><p>The time at which a particular phase of a seismic wave arrives at a station.</p>
</dd>
<dt id="term-asthenosphere">asthenosphere<a class="headerlink" href="#term-asthenosphere" title="Permalink to this term"></a></dt><dd><p>The ductile part of the Earth, just below the brittle <a class="reference internal" href="#term-lithosphere"><span class="xref std std-term">lithosphere</span></a>,
in the upper mantle. The lithosphere/asthenosphere reaches down to about 200 km.</p>
</dd>
<dt id="term-azimuth">azimuth<a class="headerlink" href="#term-azimuth" title="Permalink to this term"></a></dt><dd><p>In general a direction measured clock-wise in degrees against north. In seismology used to
measure the direction from a seismic source to a seismic station recording this event.</p>
</dd>
<dt id="term-beam">beam<a class="headerlink" href="#term-beam" title="Permalink to this term"></a></dt><dd><p>The sum of signals observed at an <a class="reference internal" href="#term-array"><span class="xref std std-term">array</span></a> shifted with respect
to the array reference coordinate assuming a particular <a class="reference internal" href="#term-slowness"><span class="xref std std-term">slowness</span></a>
and <a class="reference internal" href="#term-azimuth"><span class="xref std std-term">azimuth</span></a>. Optimum values for slowness and azimuth can be
found, e.g. by <a class="reference internal" href="#term-F-K"><span class="xref std std-term">F-K</span></a> analysis.</p>
</dd>
<dt id="term-beam-packing">beam packing<a class="headerlink" href="#term-beam-packing" title="Permalink to this term"></a></dt><dd><p>Equivalent to the <a class="reference internal" href="#term-F-K"><span class="xref std std-term">F-K</span></a> analysis where the <a class="reference internal" href="#term-beam"><span class="xref std std-term">beam</span></a> and the related
parameters such as <a class="reference internal" href="#term-beam-power"><span class="xref std std-term">beam power</span></a> or <a class="reference internal" href="#term-semblance"><span class="xref std std-term">semblance</span></a> are formed in the
time domain. Seismograms from the <a class="reference internal" href="#term-array"><span class="xref std std-term">array</span></a> stations are shifted according
to the considered ranges of <a class="reference internal" href="#term-slowness"><span class="xref std std-term">slowness</span></a> and <a class="reference internal" href="#term-backazimuth"><span class="xref std std-term">backazimuth</span></a> or
<a class="reference internal" href="#term-wave-number"><span class="xref std std-term">wave number</span></a> and summed to form the beam.</p>
</dd>
<dt id="term-beam-power">beam power<a class="headerlink" href="#term-beam-power" title="Permalink to this term"></a></dt><dd><p>The energy of <a class="reference internal" href="#term-beam"><span class="xref std std-term">beam</span></a> within a defined time window.</p>
</dd>
<dt id="term-backazimuth">backazimuth<a class="headerlink" href="#term-backazimuth" title="Permalink to this term"></a></dt><dd><p>The direction from the seismic station towards a seismic source, measured in degrees clock-wise
against north; sometimes also just called azimuth.</p>
</dd>
<dt id="term-Benioff-zone">Benioff zone<a class="headerlink" href="#term-Benioff-zone" title="Permalink to this term"></a></dt><dd><p>see <a class="reference internal" href="#term-Wadati-Benioff-zone"><span class="xref std std-term">Wadati-Benioff zone</span></a></p>
</dd>
<dt id="term-body-wave">body wave<a class="headerlink" href="#term-body-wave" title="Permalink to this term"></a></dt><dd><p>A seismic wave that propagates through the interior of the Earth, as opposed to
surface waves that propagate near the Earths surface. <a class="reference internal" href="#term-P-wave"><span class="xref std std-term">P</span></a> and <a class="reference internal" href="#term-S-wave"><span class="xref std std-term">S waves</span></a>, which shake
the ground in different ways, are examples.</p>
</dd>
<dt id="term-body-wave-magnitude">body wave magnitude<a class="headerlink" href="#term-body-wave-magnitude" title="Permalink to this term"></a></dt><dd><p>see <a class="reference internal" href="#term-magnitude-body-wave-mb"><span class="xref std std-term">magnitude, body-wave (mb)</span></a></p>
</dd>
<dt id="term-calibration">calibration<a class="headerlink" href="#term-calibration" title="Permalink to this term"></a></dt><dd><p>The process of determining the response function (distortion of the input signal) and
sensitivity of an instrument or its derived component.</p>
</dd>
<dt id="term-CAV">CAV<a class="headerlink" href="#term-CAV" title="Permalink to this term"></a></dt><dd><p>cumulated absolute velocity</p>
</dd>
<dt id="term-CI">CI<a class="headerlink" href="#term-CI" title="Permalink to this term"></a></dt><dd><p>Characteristic Intensity</p>
</dd>
<dt id="term-channel-code">channel code<a class="headerlink" href="#term-channel-code" title="Permalink to this term"></a></dt><dd><p>Description of characteristics of data related to the recording sensor and
data logger as well as instrument responses, sampling frequencies, etc.
The standard codes are defined in the <span id="id2"><em>SEED Reference Manual</em> [<a class="reference internal" href="references.html#id252" title="SEED Reference Manual. USGS, 2012. URL: http://www.fdsn.org/pdf/SEEDManual_V2.4.pdf.">31</a>]</span>.</p>
</dd>
<dt id="term-Circum-Pacific-belt">Circum-Pacific belt<a class="headerlink" href="#term-Circum-Pacific-belt" title="Permalink to this term"></a></dt><dd><p>The zone surrounding the Pacific Ocean that is characterized by frequent and strong
earthquakes and many volcanoes as well as high tsunami hazard. Also called the Ring of Fire.</p>
</dd>
<dt id="term-coda">coda<a class="headerlink" href="#term-coda" title="Permalink to this term"></a></dt><dd><p>The tail of a seismic signal, usually with exponentially decaying amplitudes, which
follow a strong wave arrival. Coda waves are due to scattering and superposition of multi-path arrivals.</p>
</dd>
<dt id="term-coda-phase">coda phase<a class="headerlink" href="#term-coda-phase" title="Permalink to this term"></a></dt><dd><p>A detection of a single phase of unknown path found within the coda signal envelope,
designated as tx, e.g. Px or Sx.</p>
</dd>
<dt id="term-coherent">coherent<a class="headerlink" href="#term-coherent" title="Permalink to this term"></a></dt><dd><p>Seismic signals detected on various seismic sensors of a seismic array or network are said to
be coherent if they are related to each other in time, amplitude and/or waveform because they
come from the same seismic source.</p>
</dd>
<dt id="term-color">color<a class="headerlink" href="#term-color" title="Permalink to this term"></a></dt><dd><p>Colors are given in hexadecimal representation or by <a class="reference internal" href="#term-color-keyword-name"><span class="xref std std-term">color keyword names</span></a>.</p>
</dd>
<dt id="term-color-keyword-name">color keyword name<a class="headerlink" href="#term-color-keyword-name" title="Permalink to this term"></a></dt><dd><p>Color keyword names allow the specification of color values by names
representing color codes instead of RGB or hexadecimal representation. Find examples
on the <a class="reference external" href="https://www.w3.org/TR/SVG11/types.html#ColorKeywords">website of W3C</a>.
Color keyword names have been introduced in SeisComP in version 4.4.0.</p>
</dd>
<dt id="term-convolution">convolution<a class="headerlink" href="#term-convolution" title="Permalink to this term"></a></dt><dd><p>A mathematically equivalent operation that describes the action of a linear (mechanical
and/or electronic) system on a signal, such as that of a filter on a seismic signal.</p>
</dd>
<dt id="term-core">core<a class="headerlink" href="#term-core" title="Permalink to this term"></a></dt><dd><p>The innermost part of the Earth. The outer core extends from about 2900 to about 5120 km below
the Earths surface and consists in its main components of a mixture of liquid iron and nickel.
The inner core is the central sphere of the Earth with a diameter of 1250 km and consists of solid metal.</p>
</dd>
<dt id="term-Core-Mantle-Boundary-CMB">Core-Mantle Boundary(CMB)<a class="headerlink" href="#term-Core-Mantle-Boundary-CMB" title="Permalink to this term"></a></dt><dd><p>see <a class="reference internal" href="#term-Gutenberg-discontinuity"><span class="xref std std-term">Gutenberg discontinuity</span></a></p>
</dd>
<dt id="term-corner-frequency">corner frequency<a class="headerlink" href="#term-corner-frequency" title="Permalink to this term"></a></dt><dd><p>The frequency at which the curve representing the Fourier amplitude spectrum of a recorded seismic
signal abruptly changes its slope. For earthquakes, this frequency is a property of the source and
related to fault size, rupture velocity, source duration and stress drop in the source. Also the
frequency at which the transfer function / magnification curve of a recording system changes its slope.</p>
</dd>
<dt id="term-creep">creep<a class="headerlink" href="#term-creep" title="Permalink to this term"></a></dt><dd><p>Slow, more or less continuous movement occurring on faults due to ongoing tectonic deformation.
Also applied to slow movement of landslide masses down a slope because of gravitational forces.
Faults that are creeping do not tend to have large earthquakes. This fault condition is commonly
referred to as unlocked.</p>
</dd>
<dt id="term-crust">crust<a class="headerlink" href="#term-crust" title="Permalink to this term"></a></dt><dd><p>The outermost major layer of the Earth, ranging from about 10 to 70 km in thickness worldwide.
The oceanic crust is thinner (about 10 to 15 km) than the continental crust (about 25 to 70 km).
The uppermost 15-35 km of the crust is brittle enough to produce earthquakes. The seismogenic crust
is separated from the lower crust by the brittle-ductile boundary. The crust is usually characterized
by P-wave velocities below 8 km/s (average velocity of about 6 km/s).</p>
</dd>
<dt id="term-delay">delay<a class="headerlink" href="#term-delay" title="Permalink to this term"></a></dt><dd><p>The time difference between the arrival time and the end time of the last record achieved plus
the half record length. The delay can be computed by <a class="reference internal" href="../apps/scqc.html#scqc"><span class="std std-ref">scqc</span></a>.</p>
</dd>
<dt id="term-depth-Phase">depth Phase<a class="headerlink" href="#term-depth-Phase" title="Permalink to this term"></a></dt><dd><p>see <a class="reference internal" href="#term-pP-phase"><span class="xref std std-term">pP phase</span></a> or <a class="reference internal" href="#term-sP-phase"><span class="xref std std-term">sP phase</span></a></p>
</dd>
<dt id="term-detection">detection<a class="headerlink" href="#term-detection" title="Permalink to this term"></a></dt><dd><p>Identification of an arrival of a seismic signal with amplitudes above and/or signal shape
(waveform) different from seismic noise.</p>
</dd>
<dt id="term-directivity">directivity<a class="headerlink" href="#term-directivity" title="Permalink to this term"></a></dt><dd><p>An effect of a propagating fault rupture whereby the amplitudes of the generated ground motions
depend on the direction of wave propagation with respect to fault orientation and slip
direction (radiation pattern). The directivity and thus the radiation pattern is different for
<a class="reference internal" href="#term-P-wave"><span class="xref std std-term">P</span></a> and <a class="reference internal" href="#term-S-wave"><span class="xref std std-term">S waves</span></a>.</p>
</dd>
<dt id="term-EDA">EDA<a class="headerlink" href="#term-EDA" title="Permalink to this term"></a></dt><dd><p>Effective Design Acceleration</p>
</dd>
<dt id="term-EIDA">EIDA<a class="headerlink" href="#term-EIDA" title="Permalink to this term"></a></dt><dd><p>European Integrated Data Archive: <a class="reference external" href="http://www.orfeus-eu.org/data/eida/">http://www.orfeus-eu.org/data/eida/</a></p>
</dd>
<dt id="term-epicenter">epicenter<a class="headerlink" href="#term-epicenter" title="Permalink to this term"></a></dt><dd><p>Vertical projection of the hypocenter to the surface.</p>
</dd>
<dt id="term-event">event<a class="headerlink" href="#term-event" title="Permalink to this term"></a></dt><dd><ol class="arabic simple">
<li><p>General term used for a localized disturbance (earthquake, explosion, etc.) which generates seismic waves.</p></li>
<li><p>QuakeML object. The event is the parent object of several <a class="reference internal" href="#term-origin"><span class="xref std std-term">origins</span></a>.
Among these origins a preferred origin
and its <a class="reference internal" href="#term-preferred-magnitude"><span class="xref std std-term">preferred magnitude</span></a> is selected to represent the event.
An event can be seen as an earthquake folder
which contains information about earthquake parameters.</p></li>
</ol>
</dd>
<dt id="term-fault-plane-solution">fault-plane solution<a class="headerlink" href="#term-fault-plane-solution" title="Permalink to this term"></a></dt><dd><p>Representation of the fault activated in an earthquake and the caused direction of slip on the fault by
a circle with two intersecting curves looking like a beach ball. A fault-plane solution is found by the
analysis of seismic records at many stations of an earthquake to obtain the radiation pattern. From the
radiation pattern the fault parameter and the slip direction are determined using a stereographic
projection or its mathematical equivalent. The most common analysis uses the direction of first motion
of P wave onsets and yields two possible orientations for the fault rupture and the direction of seismic
slip. Another technique is to use the polarization of teleseismic <a class="reference internal" href="#term-S-wave"><span class="xref std std-term">S waves</span></a> and/or to measure amplitude
ratios between different phase types. Further inferences can be made from these data concerning the
principal axes of stress in the region of the earthquake. The principal stress axes determined by this
method are the compressional axis (also called the P-axis, i.e. the axis of greatest compression, or s1),
the tensional axis (also known as the T-axis, i.e., the axis of least compression, or s3), and the
intermediate axis (s2).</p>
</dd>
<dt id="term-filter-ing">filter(ing)<a class="headerlink" href="#term-filter-ing" title="Permalink to this term"></a></dt><dd><p>A filter attenuates certain frequencies of a (seismic) signal and amplifies others. The process of
filtering can be accomplished electronically while recording or numerically in a computer. Filtering also
occurs naturally as seismic energy passes through the Earth.</p>
<p>The available and integrated filters in <cite>SeisComP</cite> are documented in <a class="reference internal" href="filter-grammar.html#filter-grammar"><span class="std std-ref">Filter Grammar</span></a>.</p>
</dd>
<dt id="term-first-motion">first motion<a class="headerlink" href="#term-first-motion" title="Permalink to this term"></a></dt><dd><p>The first noticeable displacement in a seismogram caused by the arrival of a P wave at the seismometer.
Upward motion of the ground at the seismometer indicates a dilatation at the source, downward motion
indicates a compression. Due to the presence of seismic noise the proper polarity of the first motion
may be difficult to recognize.</p>
</dd>
<dt id="term-F-K">F-K<a class="headerlink" href="#term-F-K" title="Permalink to this term"></a></dt><dd><p>F-K refers to a 2-D <a class="reference internal" href="#term-Fourier-analysis"><span class="xref std std-term">Fourier analysis</span></a> where the base functions
are defined, e.g. by ranges of <a class="reference internal" href="#term-frequency"><span class="xref std std-term">frequency</span></a> and <a class="reference internal" href="#term-wave-number"><span class="xref std std-term">wave number</span></a>.
F-K analysis is applied for signal detection by transforming time series
recorded at several sensors, e.g. seismic or infrasound <a class="reference internal" href="#term-array"><span class="xref std std-term">array</span></a>
stations to the time and space domain.</p>
<p>The equivalent to F-K analysis in the time domain is <a class="reference internal" href="#term-beam-packing"><span class="xref std std-term">beam packing</span></a>.</p>
</dd>
<dt id="term-focal-mechanism">focal mechanism<a class="headerlink" href="#term-focal-mechanism" title="Permalink to this term"></a></dt><dd><p>see <a class="reference internal" href="#term-fault-plane-solution"><span class="xref std std-term">fault-plane solution</span></a></p>
</dd>
<dt id="term-foreshocks">foreshocks<a class="headerlink" href="#term-foreshocks" title="Permalink to this term"></a></dt><dd><p>Earthquakes that occur in a series of earthquakes before the largest earthquake, termed the mainshock.
Foreshocks may precede the mainshock by seconds to weeks and usually originate at or near the focus
of the larger earthquake. Not all mainshocks have foreshocks.</p>
</dd>
<dt id="term-Fourier-spectrum">Fourier spectrum<a class="headerlink" href="#term-Fourier-spectrum" title="Permalink to this term"></a></dt><dd><p>The relative amplitudes (and phase angles) at different frequencies that are derived from a time series
by Fourier analysis.</p>
</dd>
<dt id="term-Fourier-analysis">Fourier analysis<a class="headerlink" href="#term-Fourier-analysis" title="Permalink to this term"></a></dt><dd><p>The mathematical operation that resolves a time series (for example, a recording of ground motion)
into a series of numbers that characterize the relative amplitude and phase components of the signal
as a function of frequency.</p>
</dd>
<dt id="term-frequency">frequency<a class="headerlink" href="#term-frequency" title="Permalink to this term"></a></dt><dd><p>Number of cycles of a repeating signal per unit time, typically per second.</p>
</dd>
<dt id="term-frequency-domain">frequency domain<a class="headerlink" href="#term-frequency-domain" title="Permalink to this term"></a></dt><dd><p>The transformation of a seismic signal from the time domain (as a seismogram) to the frequency
domain is conducted by a <a class="reference internal" href="#term-Fourier-analysis"><span class="xref std std-term">Fourier analysis</span></a>. The signal is represented in the frequency domain by
the amplitude and phase components as a function of frequency (see spectrum). The representations of
a seismic signal in the time and in the frequency domain are equivalent in a mathematical sense.
For some procedures of data analysis the time-domain representation of a seismic record is more
suitable while for others the frequency-domain approach is more appropriate and efficient.</p>
</dd>
<dt id="term-gempa-GmbH">gempa GmbH<a class="headerlink" href="#term-gempa-GmbH" title="Permalink to this term"></a></dt><dd><p><a class="reference external" href="http://www.gempa.de/">gempa GmbH</a> is a spin-off from <a class="reference internal" href="#term-GFZ"><span class="xref std std-term">GFZ</span></a>
offering a range of services and products to monitor, process and analyze
seismicity. It is the main development and service company for <cite>SeisComP</cite>.</p>
</dd>
<dt id="term-GEOFON">GEOFON<a class="headerlink" href="#term-GEOFON" title="Permalink to this term"></a></dt><dd><p>GEOFON (<a class="reference external" href="https://geofon.gfz-potsdam.de">https://geofon.gfz-potsdam.de</a>) is part of the Modular Earth Science
Infrastructure (MESI) at <a class="reference internal" href="#term-GFZ"><span class="xref std std-term">GFZ</span></a>.</p>
</dd>
<dt id="term-geometrical-spreading">geometrical spreading<a class="headerlink" href="#term-geometrical-spreading" title="Permalink to this term"></a></dt><dd><p>The component of reduction in wave amplitude due to the radial spreading of seismic energy with
increasing distance from a given source.</p>
</dd>
<dt id="term-GFZ">GFZ<a class="headerlink" href="#term-GFZ" title="Permalink to this term"></a></dt><dd><p>Helmholtz Centre Potsdam <a class="reference external" href="http://www.gfz-potsdam.de/">German Research Centre for Geosciences</a>.
<cite>SeisComP</cite> was originally developed at GFZ.</p>
</dd>
<dt id="term-GMPE">GMPE<a class="headerlink" href="#term-GMPE" title="Permalink to this term"></a></dt><dd><p>Ground Motion Prediction Equation</p>
</dd>
<dt id="term-Green-s-function">Greens function<a class="headerlink" href="#term-Green-s-function" title="Permalink to this term"></a></dt><dd><p>A mathematical representation that, in reference to earthquake shaking, is used to represent the
ground motion caused by instantaneous slip on a small part of a fault. Greens functions can be
summed over a large fault surface to compute the ground shaking for a large earthquake rupturing
a fault of finite size. The fractional fault-slip events that are summed can be records from
small earthquakes on the fault or they can be theoretically computed small-earthquake records.</p>
</dd>
<dt id="term-Gutenberg-discontinuity">Gutenberg discontinuity<a class="headerlink" href="#term-Gutenberg-discontinuity" title="Permalink to this term"></a></dt><dd><p>The seismic velocity discontinuity marking the core-mantle boundary (CMB) at which the velocity
of P waves drops from about 13.7 km/s to about 8.0 km/s and the velocity of <a class="reference internal" href="#term-S-wave"><span class="xref std std-term">S waves</span></a> drops from
about 7.3 km/s to 0 km/s. The CMB reflects the change from the solid mantle material to the
fluid outer core.</p>
</dd>
<dt id="term-GUI">GUI<a class="headerlink" href="#term-GUI" title="Permalink to this term"></a></dt><dd><p>Graphical use interface, e.g. <a class="reference internal" href="../apps/scolv.html#scolv"><span class="std std-ref">scolv</span></a>.</p>
</dd>
<dt id="term-hypocenter">hypocenter<a class="headerlink" href="#term-hypocenter" title="Permalink to this term"></a></dt><dd><p>Coordinates of an earthquake point source. Hypocenters based on <a class="reference internal" href="#term-P-wave"><span class="xref std std-term">P</span></a> and <a class="reference internal" href="#term-S-wave"><span class="xref std std-term">S wave</span></a>
first arrivals point to the place where the rupture process starts. For large earthquakes the
source location determined by <a class="reference internal" href="#term-P-wave"><span class="xref std std-term">P wave</span></a> first arrivals can differ significantly from the location of
maximum energy release.</p>
</dd>
<dt id="term-Ia">Ia<a class="headerlink" href="#term-Ia" title="Permalink to this term"></a></dt><dd><p>Arias Intensity</p>
</dd>
<dt id="term-infrasound-array">infrasound array<a class="headerlink" href="#term-infrasound-array" title="Permalink to this term"></a></dt><dd><p>An <a class="reference internal" href="#term-array"><span class="xref std std-term">array</span></a> of barometers measuring infrasound signals.</p>
</dd>
<dt id="term-intensity">intensity<a class="headerlink" href="#term-intensity" title="Permalink to this term"></a></dt><dd><p>A measure of the effects of an earthquake at a particular place at the Earths surface on humans
and (or) structures. The intensity at a point depends not only upon the strength of the earthquake
(magnitude) but also upon the distance from the earthquake, the depth of the hypocenter and the
local geology at that point. Several scales exist, most of them giving the intensity in 12 degrees,
usually written as Roman numerals. Most frequently used are at present the European Macroseismic
Scale (EMS-98), and in the United States the Modified Mercalli scale and the Rossi-Forel scale.
There are many different intensity values for one earthquake, depending on how far you are away
from the epicenter; this is unlike the magnitude value, which is one number for each earthquake
as a measure of the amount of seismic wave energy released by it.</p>
</dd>
<dt id="term-interplate-intraplate">interplate/intraplate<a class="headerlink" href="#term-interplate-intraplate" title="Permalink to this term"></a></dt><dd><p>Intraplate pertains to processes within the Earths crustal plates. Interplate pertains to
processes between the plates.</p>
</dd>
<dt id="term-interplate-coupling">interplate coupling<a class="headerlink" href="#term-interplate-coupling" title="Permalink to this term"></a></dt><dd><p>The qualitative ability of a subduction thrust fault to lock and accumulate stress. Strong
interplate coupling implies that the fault is locked and capable of accumulation stress whereas
weak coupling implies that the fault is unlocked or only capable of accumulating low stress.
A fault with weak interplate coupling could be aseismic or could slip by creep.</p>
</dd>
<dt id="term-inventory">inventory<a class="headerlink" href="#term-inventory" title="Permalink to this term"></a></dt><dd><p>The inventory is the collection of all available meta data related to <a class="reference internal" href="#term-network"><span class="xref std std-term">network</span></a>,
<a class="reference internal" href="#term-station"><span class="xref std std-term">station</span></a>, <a class="reference internal" href="#term-location-code"><span class="xref std std-term">location code</span></a>, station <a class="reference internal" href="#term-channel-code"><span class="xref std std-term">channel code</span></a>,
characteristics of sensors and data loggers, etc. More details are given in
the concepts section <a class="reference internal" href="concepts/inventory.html#concepts-inventory"><span class="std std-ref">Inventory</span></a>.</p>
</dd>
<dt id="term-latency">latency<a class="headerlink" href="#term-latency" title="Permalink to this term"></a></dt><dd><p>Time difference between the end times of consecutive records.
The latency can be computed by <a class="reference internal" href="../apps/scqc.html#scqc"><span class="std std-ref">scqc</span></a>.</p>
</dd>
<dt id="term-lithosphere">lithosphere<a class="headerlink" href="#term-lithosphere" title="Permalink to this term"></a></dt><dd><p>The outer solid part of the Earth, including crust and uppermost mantle. The lithosphere is
about 100 km thick, although its thickness is age-dependent (older lithosphere is thicker).
At some locations the lithosphere below the crust is brittle enough to produce earthquakes by
faulting, such as within a subducted oceanic plate.</p>
</dd>
<dt id="term-location-code">location code<a class="headerlink" href="#term-location-code" title="Permalink to this term"></a></dt><dd><p>Description of particular sensor location associated to a station. The standard
location codes are defined in the <span id="id3"><em>SEED Reference Manual</em> [<a class="reference internal" href="references.html#id252" title="SEED Reference Manual. USGS, 2012. URL: http://www.fdsn.org/pdf/SEEDManual_V2.4.pdf.">31</a>]</span>.</p>
</dd>
<dt id="term-Love-wave">Love wave<a class="headerlink" href="#term-Love-wave" title="Permalink to this term"></a></dt><dd><p>A major type of surface waves having a horizontal motion that is transverse (or perpendicular)
to the direction of propagation. It is named after A. E. H. Love, the English mathematician
who discovered it.</p>
</dd>
<dt id="term-leaky-mode">leaky mode<a class="headerlink" href="#term-leaky-mode" title="Permalink to this term"></a></dt><dd><p>A seismic surface wave which is imperfectly trapped, e.g., within a low-velocity layer or a
sequence of layers, so that its energy leaks or escapes across a layer boundary causing some
attenuation.</p>
</dd>
<dt id="term-low-velocity-layer-zone">low-velocity layer/zone<a class="headerlink" href="#term-low-velocity-layer-zone" title="Permalink to this term"></a></dt><dd><p>Any layer in the Earth in which seismic wave velocities are lower than in the layers above and below.</p>
</dd>
<dt id="term-magnification-curve">magnification curve<a class="headerlink" href="#term-magnification-curve" title="Permalink to this term"></a></dt><dd><p>A diagram showing the dependence of amplification, e.g. of the seismic ground motion by a
seismograph, as a function of frequency.</p>
</dd>
<dt id="term-magnitude">magnitude<a class="headerlink" href="#term-magnitude" title="Permalink to this term"></a></dt><dd><p>A number that characterizes the relative size of an earthquake. The magnitude is based on
<a class="reference internal" href="#term-amplitude"><span class="xref std std-term">amplitude</span></a> measurement of the maximum motion recorded by a seismograph
(sometimes for waves of a particular frequency),
corrected for the attenuation with distance. Several scales have been defined, but the most commonly used are:</p>
<ol class="arabic simple">
<li><p>local magnitude (ML), commonly referred to as “Richter magnitude”</p></li>
<li><p>surface-wave magnitude (Ms)</p></li>
<li><p>body-wave magnitude (mb)</p></li>
<li><p>moment magnitude (Mw).</p></li>
</ol>
<p>The magnitude scales 1-3 have limited range and applicability and do not
satisfactorily measure the
size of the largest earthquakes. The moment magnitude (Mw) scale, based on
the concept of seismic moment,
is uniformly applicable to all earthquake sizes but is more difficult to
compute than the other types. In
principal, all magnitude scales could be cross calibrated to yield the same
value for any given earthquake, but
this expectation has proven to be only approximately true, thus the
magnitude type as well as its value is needed to be specified.</p>
<p>Additional or modified magnitudes can be computed by providing plugins.</p>
<p>In <cite>SeisComP</cite> magnitudes are computed automatically by <a class="reference internal" href="../apps/scmag.html#scmag"><span class="std std-ref">scmag</span></a> or interactively
by <a class="reference internal" href="../apps/scolv.html#scolv"><span class="std std-ref">scolv</span></a>.</p>
</dd>
<dt id="term-magnitude-local-ML">magnitude, local (ML)<a class="headerlink" href="#term-magnitude-local-ML" title="Permalink to this term"></a></dt><dd><p>Magnitude scale introduced by Richter in the early 1930s (<span id="id4">Richter [<a class="reference internal" href="references.html#id62" title="C.F. Richter. An instrumental earthquake magnitude scale. Bull. Seismol. Soc. Am., 1:1 - 32, 1935. URL: https://resolver.caltech.edu/CaltechAUTHORS:20140804-143558638, doi:10.1785/BSSA0250010001.">57</a>]</span>)
to have a common scale for the strength of earthquakes. The basic observation
is the systematic decay of the logarithm of the maximum
amplitudes with increasing distance for different earthquakes described by:</p>
<div class="math">
<p><img src="../_images/math/b0ebe6e979dee4886949b4cda7beda6170c120d0.png" alt="ML = \log A_{max} - \log A_0"/></p>
</div><p>with A<sub>0</sub> as amplitude of a reference event. For the reference event
ML = 0 the formula can be rewritten to</p>
<div class="math">
<p><img src="../_images/math/c2480e17e843eda90dd925a3cfb2923484409583.png" alt="ML = \log A_{max} - 2.48 + 2.76 \log \Delta"/></p>
</div><p>with Δ being the distance of the station to the earthquake location. ML is a
magnitude scale for
recordings of earthquakes smaller than ML 7 at regional stations. It is
usually a measure of the
regional-distance S-wave on horizontal component records.
The original formula is only valid for records from a <a class="reference internal" href="#term-Wood-Anderson-seismometer"><span class="xref std std-term">Wood-Anderson torsion
seismometer</span></a> with a natural period of
0.8 s and shallow earthquakes in California. Therefore calibration functions
for other regions and wider depth ranges are necessary.
A <a class="reference internal" href="#term-Wood-Anderson-seismometer"><span class="xref std std-term">Wood-Anderson torsion seismometer</span></a> is
simulated when measuring amplitudes.</p>
<p>For amplitudes measured on the vertical component records, additional
correction factors have to be applied. ML saturates at
magnitudes around 7 because the maximum amplitudes of larger earthquakes
occur at longer periods than
the bandpass of 0.1 s and 3 s for the magnitude calculation.</p>
<p>In <cite>SeisComP</cite> a modified local magnitude
<a class="reference internal" href="#term-magnitude-local-vertical-MLv"><span class="xref std std-term">MLv</span></a> is determined by simulation
of a Wood-Anderson instrument and then measuring the amplitude in a 150 s
time window on the vertical component of station with distances smaller than 8°.</p>
<ul class="simple">
<li><p>Amplitude unit in <cite>SeisComP</cite>: <strong>millimeter</strong> (mm)</p></li>
</ul>
<p>Read the <a class="reference internal" href="../apps/global_ml.html#global-ml"><span class="std std-ref">technical documentation</span></a> for more details and
the configuration.</p>
</dd>
<dt id="term-magnitude-local-custom-MLc">magnitude, local custom (MLc)<a class="headerlink" href="#term-magnitude-local-custom-MLc" title="Permalink to this term"></a></dt><dd><p>The local magnitude measured on the horizontal components with
custom parametric or non-parametric function, configurable amplitude
filtering, <a class="reference internal" href="#term-Wood-Anderson-seismometer"><span class="xref std std-term">Wood-Anderson torsion seismometer</span></a> and distance measures.</p>
<ul class="simple">
<li><p>Amplitude unit in <cite>SeisComP</cite>: <strong>millimeter</strong> (mm)</p></li>
</ul>
<p>Read the <a class="reference internal" href="../apps/global_mlc.html#global-mlc"><span class="std std-ref">technical documentation</span></a> for more details and
the configuration.</p>
</dd>
<dt id="term-magnitude-local-horizontal-MLh">magnitude, local horizontal (MLh)<a class="headerlink" href="#term-magnitude-local-horizontal-MLh" title="Permalink to this term"></a></dt><dd><p>The local magnitude computed from amplitudes measured on the horizontal
components with a modified parametric calibration function as compared to
<a class="reference internal" href="#term-magnitude-local-ML"><span class="xref std std-term">ML</span></a>.</p>
<ul class="simple">
<li><p>Amplitude unit in <cite>SeisComP</cite>: <strong>millimeter</strong> (mm)</p></li>
</ul>
<p>Read the <a class="reference internal" href="../apps/global_mlh.html#global-mlh"><span class="std std-ref">technical documentation</span></a> for more details and
the configuration.</p>
</dd>
<dt id="term-magnitude-local-GNS-GEONET-MLr">magnitude, local GNS/GEONET (MLr)<a class="headerlink" href="#term-magnitude-local-GNS-GEONET-MLr" title="Permalink to this term"></a></dt><dd><p>Local magnitude calculated from <a class="reference internal" href="#term-magnitude-local-vertical-MLv"><span class="xref std std-term">MLv</span></a>
amplitudes based on GNS/GEONET specifications for New Zealand.</p>
<p>Read the <a class="reference internal" href="../apps/global_mlr.html#global-mlr"><span class="std std-ref">technical documentation</span></a> for more details and the configuration.</p>
</dd>
<dt id="term-magnitude-local-vertical-MLv">magnitude, local vertical (MLv)<a class="headerlink" href="#term-magnitude-local-vertical-MLv" title="Permalink to this term"></a></dt><dd><p>The <a class="reference internal" href="#term-magnitude-local-ML"><span class="xref std std-term">ML</span></a> magnitude with amplitudes measured on
the vertical component instead of the horizontals.</p>
<ul class="simple">
<li><p>Amplitude unit in <cite>SeisComP</cite>: <strong>millimeter</strong> (mm)</p></li>
</ul>
<p>Read the <a class="reference internal" href="../apps/global_mlv.html#global-mlv"><span class="std std-ref">technical documentation</span></a> for more details and the configuration.</p>
</dd>
<dt id="term-magnitude-Nuttli-MN">magnitude, Nuttli (MN)<a class="headerlink" href="#term-magnitude-Nuttli-MN" title="Permalink to this term"></a></dt><dd><p>Nuttli magnitude for Canada and other Cratonic regions.</p>
<ul class="simple">
<li><p>Amplitude unit in <cite>SeisComP</cite>: <strong>meter/second</strong> (m/s)</p></li>
</ul>
<p>Read the <a class="reference internal" href="../apps/global_mn.html#global-mn"><span class="std std-ref">technical documentation</span></a> for more details and the configuration.</p>
</dd>
<dt id="term-magnitude-body-wave-mb">magnitude, body-wave (mb)<a class="headerlink" href="#term-magnitude-body-wave-mb" title="Permalink to this term"></a></dt><dd><p>Magnitude developed for teleseismic body waves. mb is defined on the amplitude
of the first few cycles of the P-wave restituted to <a class="reference internal" href="#term-WWSSN_SP"><span class="xref std std-term">WWSSN_SP</span></a>.</p>
<ul class="simple">
<li><p>Amplitude unit in <cite>SeisComP</cite>: <strong>nanometer</strong> (nm)</p></li>
</ul>
<p>Read the <a class="reference internal" href="../apps/global_mb.html#global-mb"><span class="std std-ref">technical documentation</span></a> for more details and the configuration.</p>
</dd>
<dt id="term-magnitude-broadband-body-wave-mB_BB">magnitude, broadband body-wave (mB_BB)<a class="headerlink" href="#term-magnitude-broadband-body-wave-mB_BB" title="Permalink to this term"></a></dt><dd><p>mB_BB is the term recommended by the IASPEI commission for
<a class="reference internal" href="#term-magnitude-broadband-body-wave-mB"><span class="xref std std-term">magnitude, broadband body-wave (mB)</span></a> which is used in <cite>SeisComP</cite>.</p>
</dd>
<dt id="term-magnitude-broadband-body-wave-mB">magnitude, broadband body-wave (mB)<a class="headerlink" href="#term-magnitude-broadband-body-wave-mB" title="Permalink to this term"></a></dt><dd><p>mB is a magnitude based on body waves like <a class="reference internal" href="#term-magnitude-body-wave-mb"><span class="xref std std-term">mb</span></a>,
but with the amplitude measured in a broad frequency range and longer time windows.
mB is used as a synonym for <a class="reference internal" href="#term-magnitude-broadband-body-wave-mB_BB"><span class="xref std std-term">mB_BB</span></a>.</p>
<ul class="simple">
<li><p>Amplitude unit in <cite>SeisComP</cite> is <strong>nanometer per second</strong> (nm/s)</p></li>
</ul>
<p>Read the <a class="reference internal" href="../apps/global_mb_bb.html#global-mb-bb"><span class="std std-ref">technical documentation</span></a> for more details and the configuration.</p>
</dd>
<dt id="term-magnitude-cumulative-body-wave-mBc">magnitude, cumulative body-wave (mBc)<a class="headerlink" href="#term-magnitude-cumulative-body-wave-mBc" title="Permalink to this term"></a></dt><dd><p>mBc is the cumulative body-wave magnitude. See <span id="id5">Bormann and Wylegalla [<a class="reference internal" href="references.html#id17" title="P. Bormann and K. Wylegalla. Quick estimator of the size of great earthquakes. EOS, 86(46):464, 2005.">40</a>]</span>
and <span id="id6">Bormann and Saul [<a class="reference internal" href="references.html#id19" title="P. Bormann and J. Saul. A Fast, Non-saturating Magnitude Estimator for Great Earthquakes. Seismol. Res. Lett., 80(5):808 - 816, 2009. doi:10.1785/gssrl.80.5.808.">39</a>]</span> for details.</p>
</dd>
<dt id="term-magnitude-surface-wave-Ms">magnitude, surface wave (Ms)<a class="headerlink" href="#term-magnitude-surface-wave-Ms" title="Permalink to this term"></a></dt><dd><p>Ms is a magnitude scale based on teleseismic surface waves. Historically, Ms
is based on measurements of
the maximum horizontal true ground motion displacement amplitudes</p>
<div class="math">
<p><img src="../_images/math/712686e0db840ef121e384b1bf28f7552b5a45a9.png" alt="A_{Hmax} =\sqrt{{A_N}^2 + {A_E}^2}"/></p>
</div><p>in the total seismogram at periods around 20 s. For shallow earthquakes the dominant
long-period signals are the surface waves. The period of 20 s corresponds to the Airy
phase, a local minimum in the group velocity dispersion curve of Rayleigh surface waves.
For measuring amplitudes a correction for the WWSSN_LP instrument response is applied.</p>
<p>The Moscow-Prague equation for surface wave magnitude is given by</p>
<div class="math">
<p><img src="../_images/math/93c80b427369a5485ba5001e33597d9ad656e040.png" alt="M_s = \log \left(\frac{A_{Hmax}}{T}\right) + 1.66 \log(\Delta) + 3.3"/></p>
</div><p>where T is the measured period.</p>
<div class="math">
<p><img src="../_images/math/e5eedbf96d0b9836511e050896a63b594690134f.png" alt="M_s = \log \left(\frac{A}{T}\right)max + 1.66 \log(\Delta) + 3.3"/></p>
</div><p>Here, the maximum ground particle velocity, (A/T)max, is used instead of the AHmax to
allow a broader spectrum of dominant periods. This formula is valid for distances of
2° to 160° and source depths smaller than 50 km.</p>
<ul class="simple">
<li><p>Amplitude unit in <cite>SeisComP</cite> is <strong>meter per second</strong> (m/s)</p></li>
</ul>
</dd>
<dt id="term-magnitude-surface-wave-Ms_20">magnitude, surface wave (Ms_20)<a class="headerlink" href="#term-magnitude-surface-wave-Ms_20" title="Permalink to this term"></a></dt><dd><p>Ms_20 is the <a class="reference internal" href="#term-magnitude-surface-wave-Ms"><span class="xref std std-term">Ms</span></a> surface-wave magnitude
at <em>T=20</em> s period based on the recommendations
by the IASPEI magnitude working group issued on 27 March, 2013.</p>
<ul class="simple">
<li><p>Amplitude unit in <cite>SeisComP</cite>: nanometer (nm)</p></li>
</ul>
<p>Read the <a class="reference internal" href="../apps/global_ms_20.html#global-ms-20"><span class="std std-ref">technical documentation</span></a> for more details and the configuration.</p>
</dd>
<dt id="term-magnitude-broadband-surface-wave-Ms-BB">magnitude, broadband surface wave (Ms(BB))<a class="headerlink" href="#term-magnitude-broadband-surface-wave-Ms-BB" title="Permalink to this term"></a></dt><dd><p>Ms(BB) is a broadband magnitude scale based on teleseismic surface waves.
In contrast to <a class="reference internal" href="#term-magnitude-surface-wave-Ms"><span class="xref std std-term">Ms</span></a>, amplitudes for Ms(BB)
are measured as the maximum on vertical true ground motion velocity seismograms without
instrument simulation or restitution.</p>
<p>The Moscow-Prague equation for surface wave magnitude is applied as given by</p>
<div class="math">
<p><img src="../_images/math/e265a2c12ff5dda233e41927cae4ead315596b47.png" alt="M_s = \log \left(\frac{A}{2\pi}\right) + 1.66 \log(\Delta) + 3.3"/></p>
</div><ul class="simple">
<li><p>Amplitude unit in <cite>SeisComP</cite>: <strong>meter per second</strong> (m/s)</p></li>
<li><p>Period range: all</p></li>
<li><p>Distance range: 2 - 160°</p></li>
<li><p>Depth range: 0 - 100 km</p></li>
<li><p>Time window: distance (km) / 3.5 km/s + 30 s</p></li>
</ul>
</dd>
<dt id="term-magnitude-duration-Md">magnitude, duration (Md)<a class="headerlink" href="#term-magnitude-duration-Md" title="Permalink to this term"></a></dt><dd><p>The duration magnitude measured on the coda wave train.</p>
<p>Read the <a class="reference internal" href="../apps/global_md.html#global-md"><span class="std std-ref">technical documentation</span></a> for more details and the configuration.</p>
</dd>
<dt id="term-magnitude-JMA-M_JMA">magnitude, JMA (M_JMA)<a class="headerlink" href="#term-magnitude-JMA-M_JMA" title="Permalink to this term"></a></dt><dd><p>M(JMA) is a magnitude similar to the Ms, but the formula is calibrated for instruments
with 5 s period at local distances. The data set for the calibration was gained by the
Japan Meteorological Agency (JMA).</p>
<div class="math">
<p><img src="../_images/math/f73ef943923c3e1057e14204950603563902e3bf.png" alt="M(JMA) = \log \sqrt{{A_N}^2 + {A_E}^2} + 1.73 \log\Delta - 0.83"/></p>
</div><p>This equation is valid for local (&lt; 2000 km) and shallow (&lt; 80 km)
earthquakes. For deeper earthquakes additional correction functions have
to be applied (<span id="id7">Katsumata [<a class="reference internal" href="references.html#id44" title="A. Katsumata. Comparison of Magnitudes Estimated by the Japan Meteorological Agency with Moment Magnitudes for Intermediate and Deep Earthquakes. Bull. Seism. Soc., 86(3):832 - 842, 1996.">49</a>]</span>).</p>
<ul class="simple">
<li><p>Amplitude unit in <cite>SeisComP</cite>: <strong>micrometer</strong> (um)</p></li>
<li><p>Time window: 150 s</p></li>
<li><p>Epicentral distance range: 0 - 20°</p></li>
<li><p>Depth range: 0 - 80 km</p></li>
</ul>
</dd>
<dt id="term-magnitude-moment-Mw">magnitude, moment (Mw)<a class="headerlink" href="#term-magnitude-moment-Mw" title="Permalink to this term"></a></dt><dd><p>The moment magnitude is a magnitude scale related to the seismic moment M<sub>0</sub> and
thus to the released seismic energy.
To obtain Mw the seismic moment is first determined, e.g. by a moment tensor inversion.
Then the Mw is gained by the following standard relationship between seismic moment
and the moment magnitude (M<sub>0</sub> in cgs units of dyn*cm):</p>
<div class="math">
<p><img src="../_images/math/b094f771f607c37cea7e1cfb617585a207516afa.png" alt="Mw = \frac{2}{3}(\log M_0 - 16.1)"/></p>
</div><p>This equation is analog to the relation between M<sub>s</sub> and M<sub>0</sub>.</p>
</dd>
<dt id="term-magnitude-averaged-moment-Mw-avg">magnitude, averaged moment (Mw(avg))<a class="headerlink" href="#term-magnitude-averaged-moment-Mw-avg" title="Permalink to this term"></a></dt><dd><p>Moment magnitude derived as a weighted average of other magnitudes.</p>
</dd>
<dt id="term-magnitude-broadband-P-wave-moment-Mwp">magnitude, broadband P-wave moment (Mwp)<a class="headerlink" href="#term-magnitude-broadband-P-wave-moment-Mwp" title="Permalink to this term"></a></dt><dd><p>The Mwp is a rapid estimate of the moment magnitude based on the
first-arrival P waves on broadband seismograph records. The displacement
seismograms of the P wave portion are considered as source time function
approximation. The seismic moment is estimated for each station by
integrating the displacement records. The combination of multiple records
results in an estimation of the moment magnitude without correction
for the source mechanism (<span id="id8">Tsuboi <em>et al.</em> [<a class="reference internal" href="references.html#id79" title="S. Tsuboi, K. Abe, K. Takano, and Y. Yamanaka. Rapid determination of Mw from broadband P waveforms. Bull. Seismol. Soc. Am., 1995. doi:10.1785/BSSA0850020606.">63</a>]</span>).</p>
<ul class="simple">
<li><p>Amplitude unit in <cite>SeisComP</cite>: <strong>nanometer times second</strong> (nm*s)</p></li>
<li><p>Time window: 95 s</p></li>
<li><p>Epicentral distance range: 5 - 105°</p></li>
</ul>
</dd>
<dt id="term-magnitude-derived-mB-Mw-mB">magnitude, derived mB (Mw(mB))<a class="headerlink" href="#term-magnitude-derived-mB-Mw-mB" title="Permalink to this term"></a></dt><dd><p>Moment magnitude derived from <a class="reference internal" href="#term-magnitude-broadband-body-wave-mB"><span class="xref std std-term">mB</span></a>
magnitudes using linear conversion:</p>
<p>Mw(mB) = 1.30 mB - 2.18</p>
</dd>
<dt id="term-magnitude-derived-Mwp-Mw-Mwp">magnitude, derived Mwp (Mw(Mwp))<a class="headerlink" href="#term-magnitude-derived-Mwp-Mw-Mwp" title="Permalink to this term"></a></dt><dd><p>Moment magnitude derived from <a class="reference internal" href="#term-magnitude-broadband-P-wave-moment-Mwp"><span class="xref std std-term">Mwp</span></a>
magnitudes using linear conversion after <span id="id9">Whitmore <em>et al.</em> [<a class="reference internal" href="references.html#id85" title="P.M. Whitmore, S. Tsuboi, B. Hirshorn, and T.J. Sokolowski. Magnitude dependent correction for Mwp. Science of Tsunami Hazards, 20(4):, 2002.">65</a>]</span>:</p>
<p>Mw(Mwp) = 1.31 Mwp - 1.91</p>
</dd>
<dt id="term-magnitude-summary-M">magnitude, summary (M)<a class="headerlink" href="#term-magnitude-summary-M" title="Permalink to this term"></a></dt><dd><p>Summary magnitude derived from multiple other magnitudes by <a class="reference internal" href="../apps/scmag.html#scmag"><span class="std std-ref">scmag</span></a>.</p>
</dd>
<dt id="term-mainshock">mainshock<a class="headerlink" href="#term-mainshock" title="Permalink to this term"></a></dt><dd><p>The largest earthquake in a sequence, sometimes preceded by one or more foreshocks,
and almost always followed by many aftershocks.</p>
</dd>
<dt id="term-mantle">mantle<a class="headerlink" href="#term-mantle" title="Permalink to this term"></a></dt><dd><p>The part of the Earths interior between the core and the crust.</p>
</dd>
<dt id="term-microearthquake">microearthquake<a class="headerlink" href="#term-microearthquake" title="Permalink to this term"></a></dt><dd><p>An earthquake that is not perceptible by man and can be recorded by seismographs only.
Typically, a microearthquake has a magnitude of 2 or less on the Richter scale.</p>
</dd>
<dt id="term-microseism">microseism<a class="headerlink" href="#term-microseism" title="Permalink to this term"></a></dt><dd><ol class="arabic simple">
<li><p>In a broader sense: A more or less continuous motion in the Earth in a wide frequency
range that is unrelated to any earthquake and caused by a variety of usually uncorrelated
(incoherent) natural and artificial (man-made) sources.</p></li>
<li><p>In a more specific sense: That part of seismic noise that is generated by wave motions
on lakes and oceans and their interaction with shores, typically with periods between
about 2 to 9 s (the stronger secondary microseisms), and 11 to 18 s (the weaker
primary microseisms).</p></li>
</ol>
</dd>
<dt id="term-miniSeed">miniSeed<a class="headerlink" href="#term-miniSeed" title="Permalink to this term"></a></dt><dd><p>miniSEED is the
standard for the exchange of seismic time series. It uses a fixed record
length and applies data compression as defined in <span id="id10"><em>SEED Reference Manual</em> [<a class="reference internal" href="references.html#id252" title="SEED Reference Manual. USGS, 2012. URL: http://www.fdsn.org/pdf/SEEDManual_V2.4.pdf.">31</a>]</span>.</p>
</dd>
<dt id="term-MMI">MMI<a class="headerlink" href="#term-MMI" title="Permalink to this term"></a></dt><dd><p>Modified Mercalli Intensity</p>
</dd>
<dt id="term-Moho">Moho<a class="headerlink" href="#term-Moho" title="Permalink to this term"></a></dt><dd><p>The abbreviation for the <a class="reference internal" href="#term-Mohorovicic-discontinuity"><span class="xref std std-term">Mohorovičić discontinuity</span></a>.</p>
</dd>
<dt id="term-Mohorovicic-discontinuity">Mohorovičić discontinuity<a class="headerlink" href="#term-Mohorovicic-discontinuity" title="Permalink to this term"></a></dt><dd><p>The discontinuity in seismic velocities that defines the boundary between crust and mantle
of the Earth. Named after the Croatian seismologist Andrija Mohorovičič (1857-1936) who
discovered it. The boundary is between 20 and 60 km deep beneath the continents and between
5 and 10 km deep beneath the ocean floor.</p>
</dd>
<dt id="term-moment-tensor">moment tensor<a class="headerlink" href="#term-moment-tensor" title="Permalink to this term"></a></dt><dd><p>Moment tensors or seismic moment tensors describe the equivalent forces
due to seismic point sources, e.g. earthquakes with rupture dimensions
much smaller than the distance at which they are observed.</p>
</dd>
<dt id="term-network">network<a class="headerlink" href="#term-network" title="Permalink to this term"></a></dt><dd><p>A set of stations typically maintained by one or more institutions and
tuned to record particular signals.</p>
</dd>
<dt id="term-network-magnitude">network magnitude<a class="headerlink" href="#term-network-magnitude" title="Permalink to this term"></a></dt><dd><ol class="loweralpha simple">
<li><p>The network magnitude is a magnitude value summarizing several <a class="reference internal" href="#term-station-magnitude"><span class="xref std std-term">station magnitude</span></a> values
of one <a class="reference internal" href="#term-origin"><span class="xref std std-term">origin</span></a>. Read the documentation of <a class="reference internal" href="../apps/scmag.html#scmag"><span class="std std-ref">scmag</span></a> for the details.</p></li>
<li><p>QuakeML object.</p></li>
</ol>
</dd>
<dt id="term-noise-seismic">noise (seismic)<a class="headerlink" href="#term-noise-seismic" title="Permalink to this term"></a></dt><dd><p>Incoherent natural or artificial perturbations caused by a diversity of agents and
distributed sources. One usually differentiates between ambient background noise and
instrumental noise. The former is due to natural (ocean waves, wind, rushing waters,
animal migration, ice movement, etc.) and/or man-made sources (traffic, machinery, etc.),
whereas instrumental (internal) noise may be due to the flicker noise of electronic
components and/or even Brownian molecular motions in mechanical components. Digital
data acquisition systems may add digitization noise due to their finite discrete
resolution (least significant digit). Very sensitive seismic recordings may contain
all these different noise components, however, usually their resolution is tuned so
that only seismic signals and to a certain degree also the ambient noise are resolved.
Disturbing noise can be reduced by selecting recording sites remote from noise sources,
installation of seismic sensors underground (e.g., in boreholes, tunnels or abandoned
mines) or by suitable filter procedures (improvement of the signal-to-noise ratio).</p>
</dd>
<dt id="term-Nyquist-frequency">Nyquist frequency<a class="headerlink" href="#term-Nyquist-frequency" title="Permalink to this term"></a></dt><dd><p>Half of the digital sampling rate. It is the minimum number of counts per second
needed to define unambiguously a particular frequency. If the seismic signal contains
energy in a frequency range above the Nyquist frequency the signal distortions are
called aliasing.</p>
</dd>
<dt id="term-onset">onset<a class="headerlink" href="#term-onset" title="Permalink to this term"></a></dt><dd><p>The first appearance of a seismic signal on a record.</p>
</dd>
<dt id="term-origin">origin<a class="headerlink" href="#term-origin" title="Permalink to this term"></a></dt><dd><ol class="arabic simple">
<li><p>Location (hypocenter), Time and strength estimation of an earthquake based on seismic
phases and amplitudes</p></li>
<li><p>QuakeML object</p></li>
</ol>
</dd>
<dt id="term-origin-time">origin time<a class="headerlink" href="#term-origin-time" title="Permalink to this term"></a></dt><dd><p>Estimated source time of an event belonging to a certain origin; describes the
rupture start time. Attribute of the QuakeML object Origin, see <a class="reference internal" href="#term-origin"><span class="xref std std-term">origin</span></a>.</p>
</dd>
<dt id="term-phase">phase<a class="headerlink" href="#term-phase" title="Permalink to this term"></a></dt><dd><ol class="arabic simple">
<li><p>A stage in periodic motion, such as wave motion or the motion of an oscillator,
measured with respect to a given initial point and expressed in angular measure.</p></li>
<li><p>A pulse of seismic energy arriving at a definite time, which passed the Earth
on a specific path.</p></li>
<li><p>Attribute of the QuakeML object Arrival, see <a class="reference internal" href="#term-arrival"><span class="xref std std-term">arrival</span></a>.</p></li>
</ol>
</dd>
<dt id="term-P-phase">P phase<a class="headerlink" href="#term-P-phase" title="Permalink to this term"></a></dt><dd><p>The P phase is the arrival of the direct P wave that traveled through the Earths
crust and mantle observed in epicentral distances up to 100°.</p>
</dd>
<dt id="term-Pdiff-phase">Pdiff phase<a class="headerlink" href="#term-Pdiff-phase" title="Permalink to this term"></a></dt><dd><p>The long-period P-wave energy can be diffracted at the CMB forming at distances larger
than 100° the Pdiff phase. The reason for the diffraction is the large reduction of the
P wave velocity at the CMB from about 13.7 km/s to 8 km/s. The amplitude of Pdiff is
relatively small. Pdiff is observed at distances where the outer core forms the “core
shadow” (see also <a class="reference internal" href="#term-PKP-phase"><span class="xref std std-term">PKP phase</span></a>).</p>
</dd>
<dt id="term-Pg-phase">Pg phase<a class="headerlink" href="#term-Pg-phase" title="Permalink to this term"></a></dt><dd><p>Pg is the direct P wave arriving first in local distances less than 100 km. For larger
distances Pn arrives first (see <a class="reference internal" href="#term-Pn-phase"><span class="xref std std-term">Pn phase</span></a> for details).</p>
</dd>
<dt id="term-PGA">PGA<a class="headerlink" href="#term-PGA" title="Permalink to this term"></a></dt><dd><p>Peak Ground Acceleration</p>
</dd>
<dt id="term-PGD">PGD<a class="headerlink" href="#term-PGD" title="Permalink to this term"></a></dt><dd><p>Peak Ground Displacement</p>
</dd>
<dt id="term-PGV">PGV<a class="headerlink" href="#term-PGV" title="Permalink to this term"></a></dt><dd><p>Peak Ground Velocity</p>
</dd>
<dt id="term-Pn-phase">Pn phase<a class="headerlink" href="#term-Pn-phase" title="Permalink to this term"></a></dt><dd><p>Pn is the P head wave along the Moho arriving first at local distances larger than
100 km (depending on the crustal thickness). Pn has usually smaller amplitudes than Pg.</p>
</dd>
<dt id="term-PcP-phase">PcP phase<a class="headerlink" href="#term-PcP-phase" title="Permalink to this term"></a></dt><dd><p>The P wave that is reflected at the CMB forms the PcP. At epicentral distances between
30° and 55° PcP is often recorded as sharp pulse.</p>
</dd>
<dt id="term-PKiKP-phase">PKiKP phase<a class="headerlink" href="#term-PKiKP-phase" title="Permalink to this term"></a></dt><dd><p>A P wave that travels through the Earths crust and mantle and is reflected at the
outer core-inner core boundary. At distances between 100° and 113° PKiKP can be the
first arrival if no Pdiff is observed.</p>
</dd>
<dt id="term-PKP-phase">PKP phase<a class="headerlink" href="#term-PKP-phase" title="Permalink to this term"></a></dt><dd><p>The direct P waves traversing the Earths crust, mantle and outer core without
reflection is called PKP. The outer core is a fluid causing a strong refraction at
the CMB into the outer core. The strong refraction of the seismic rays into the
core causes a “core shadow” that commences at epicentral distances of around 100° and
stretches to around 140°. Only Pdiff can be observed in this distance range. PKP is
the first arrival at distances larger than around 143°. At a distance of 144° P waves
with several paths through the Earths core arrive at the same time (caustic) and
form a strong arrival.</p>
</dd>
<dt id="term-PP-phase">PP phase<a class="headerlink" href="#term-PP-phase" title="Permalink to this term"></a></dt><dd><p>PP is a reflected P wave at the Earths surface traversing the Earths crust and mantle.</p>
</dd>
<dt id="term-pP-phase">pP phase<a class="headerlink" href="#term-pP-phase" title="Permalink to this term"></a></dt><dd><p>A P wave that has a takeoff angle of greater than 90° at the source and therefore
is first reflected at the surface near the epicenter. The pP is a depth phase.
For shallow events and at teleseismic distances pP has nearly the same path as the P wave except
for the path from hypocenter of the earthquake to the reflection point at the surface.</p>
</dd>
<dt id="term-SEED">SEED<a class="headerlink" href="#term-SEED" title="Permalink to this term"></a></dt><dd><p>Standard for the Exchange of Earthquake Data, a data format for seismological
data and metadata (<a class="reference internal" href="#term-inventory"><span class="xref std std-term">inventory</span></a>).
It is controlled as a standard by the International Federation
of Digital Seismograph Networks (FDSN).
The current version is 2.4, updated August 2012.
Read <span id="id11"><em>SEED Reference Manual</em> [<a class="reference internal" href="references.html#id252" title="SEED Reference Manual. USGS, 2012. URL: http://www.fdsn.org/pdf/SEEDManual_V2.4.pdf.">31</a>]</span> for details.</p>
</dd>
<dt id="term-S-phase">S phase<a class="headerlink" href="#term-S-phase" title="Permalink to this term"></a></dt><dd><p>The S phase is the arrival of the direct <a class="reference internal" href="#term-S-wave"><span class="xref std std-term">S wave</span></a> that traveled through the Earths
crust and mantle observed in epicentral distances up to 100°.</p>
</dd>
<dt id="term-Sg-phase">Sg phase<a class="headerlink" href="#term-Sg-phase" title="Permalink to this term"></a></dt><dd><p>Sg is the direct <a class="reference internal" href="#term-S-wave"><span class="xref std std-term">S wave</span></a> arriving first in local distances less than 100 km. For larger
distances Sn arrives first (see <a class="reference internal" href="#term-Sn-phase"><span class="xref std std-term">Sn phase</span></a> for details).</p>
</dd>
<dt id="term-Sn-phase">Sn phase<a class="headerlink" href="#term-Sn-phase" title="Permalink to this term"></a></dt><dd><p>Sn is the S head wave along the Moho arriving first at local distances larger than
100 km (depending on the crustal thickness). Sn has usually smaller amplitudes than Sg.</p>
</dd>
<dt id="term-sP-phase">sP phase<a class="headerlink" href="#term-sP-phase" title="Permalink to this term"></a></dt><dd><p>A P wave starting as an <a class="reference internal" href="#term-S-phase"><span class="xref std std-term">S phase</span></a> at the source and arriving as P.
The S phase has a takeoff angle greater than 90° at the source and therefore
is first reflected at the surface near the epicenter and then converted into
a <a class="reference internal" href="#term-P-wave"><span class="xref std std-term">P wave</span></a> phase. The sP is therefore a depth phase. For shallow
events and at teleseismic distances sP has nearly the same path as the P
wave except for the path from hypocenter of the earthquake to the
reflection point at the surface.</p>
</dd>
<dt id="term-pick">pick<a class="headerlink" href="#term-pick" title="Permalink to this term"></a></dt><dd><ol class="arabic simple">
<li><p>Automatic or manual determined phase onset</p></li>
<li><p>QuakeML object</p></li>
</ol>
</dd>
<dt id="term-polarity">polarity<a class="headerlink" href="#term-polarity" title="Permalink to this term"></a></dt><dd><p>In seismology the direction of first motion on a seismogram, either up (positive, compression)
or down (negative, dilatation or relaxation).</p>
</dd>
<dt id="term-polarization">polarization<a class="headerlink" href="#term-polarization" title="Permalink to this term"></a></dt><dd><p>The shape and orientation in space of the ground-motion particle trajectory. It differs
for different types of seismic waves such as P, S and surface waves and may be ± linear
or elliptical, prograde or retrograde. It is also influenced by heterogeneities and
anisotropy of the medium in which the seismic waves propagate and depends on their
frequency or wavelength, respectively. The polarization of ground motion may be reconstructed
by analyzing three-component seismic recordings.</p>
</dd>
<dt id="term-preferred-magnitude">preferred magnitude<a class="headerlink" href="#term-preferred-magnitude" title="Permalink to this term"></a></dt><dd><ol class="arabic simple">
<li><p>The network magnitude representing the strength of an event best as
automatically selected by <a class="reference internal" href="../apps/scevent.html#scevent"><span class="std std-ref">scevent</span></a> or interactively.</p></li>
<li><p>Attribute of the QuakeML object Event, see <a class="reference internal" href="#term-event"><span class="xref std std-term">event</span></a>.</p></li>
</ol>
</dd>
<dt id="term-preferred-origin">preferred origin<a class="headerlink" href="#term-preferred-origin" title="Permalink to this term"></a></dt><dd><ol class="arabic simple">
<li><p>The origin representing the location of an event best; generally, the location based
on the most picks or reviewed/revised by an operator. The preferred origins
is automatically selected by <a class="reference internal" href="../apps/scevent.html#scevent"><span class="std std-ref">scevent</span></a> or interactively.</p></li>
<li><p>Attribute of the QuakeML object Event, see <a class="reference internal" href="#term-event"><span class="xref std std-term">event</span></a>.</p></li>
</ol>
</dd>
<dt id="term-QuakeML">QuakeML<a class="headerlink" href="#term-QuakeML" title="Permalink to this term"></a></dt><dd><p>A XML scheme developed as an open standard for seismological meta data
exchange (<a class="reference external" href="http://www.quakeml.org">http://www.quakeml.org</a>).</p>
</dd>
<dt id="term-radiation-pattern">radiation pattern<a class="headerlink" href="#term-radiation-pattern" title="Permalink to this term"></a></dt><dd><p>Dependence of the amplitudes of seismic <a class="reference internal" href="#term-P-wave"><span class="xref std std-term">P</span></a> and <a class="reference internal" href="#term-S-wave"><span class="xref std std-term">S waves</span></a> on the direction and take-off
angle under which their seismic rays have left the seismic source. It is controlled
by the type of source mechanism, e.g., the orientation of the earthquake fault plane
and slip direction in space.</p>
</dd>
<dt id="term-Rayleigh-wave">Rayleigh wave<a class="headerlink" href="#term-Rayleigh-wave" title="Permalink to this term"></a></dt><dd><p>A seismic surface wave causing a retrograde, elliptical motion of a particle at the free
surface, with no transverse motion. It is named after Lord Rayleigh (1842-1919), who
predicted its existence.</p>
</dd>
<dt id="term-ray-theory">ray theory<a class="headerlink" href="#term-ray-theory" title="Permalink to this term"></a></dt><dd><p>Theoretical approach, which treats wave propagation as the propagation of seismic rays.
It is an approximation, which yields good results for short wave length (high-frequency
approximation) and allows easy calculations of travel times.</p>
</dd>
<dt id="term-ray-tracing-method">ray-tracing method<a class="headerlink" href="#term-ray-tracing-method" title="Permalink to this term"></a></dt><dd><p>Computational method of calculating ground-shaking estimates that assumes that the
ground motion is composed of multiple arrivals of seismic rays and related energy
bundles (Gauss beams) that leave the source and are reflected or refracted at velocity
boundaries according to Snells Law. The amplitudes of reflected and refracted waves
at each boundary are recalculated according to the Law of Conservation of Energy.</p>
</dd>
<dt id="term-recurrence-interval">recurrence interval<a class="headerlink" href="#term-recurrence-interval" title="Permalink to this term"></a></dt><dd><p>The average time span between large earthquakes at a particular site. Also
termed return period.</p>
</dd>
<dt id="term-reflection">reflection<a class="headerlink" href="#term-reflection" title="Permalink to this term"></a></dt><dd><p>The energy or wave from a seismic source that has been returned (reflected) from an
interface between materials of different elastic properties within the Earth, just
as a mirror reflects light.</p>
</dd>
<dt id="term-refraction">refraction<a class="headerlink" href="#term-refraction" title="Permalink to this term"></a></dt><dd><p>The deflection, or bending, of the ray path of a seismic wave caused by its passage
from one material to another having different elastic properties.</p>
<p>Bending of a tsunami wave front owing to variations in the water depth along a coastline.</p>
</dd>
<dt id="term-relaxation-theory">relaxation theory<a class="headerlink" href="#term-relaxation-theory" title="Permalink to this term"></a></dt><dd><p>A concept in which radiated seismic energy is released from stored strain energy
during the slip along a fault until the adjacent fault blocks reach a new state of equilibrium.</p>
</dd>
<dt id="term-residual">residual<a class="headerlink" href="#term-residual" title="Permalink to this term"></a></dt><dd><ol class="arabic simple">
<li><p>The difference between the measured and predicted values of some quantity (e.g., theoretical
and measured phase arrival time).</p></li>
<li><p>Attribute of QuakeML object Arrival, see <a class="reference internal" href="#term-arrival"><span class="xref std std-term">arrival</span></a>.</p></li>
</ol>
</dd>
<dt id="term-Ring-of-Fire">Ring of Fire<a class="headerlink" href="#term-Ring-of-Fire" title="Permalink to this term"></a></dt><dd><p>The zone of volcanoes and earthquakes surrounding the Pacific Ocean which is called
the Circum-Pacific belt; about 90% of the worlds earthquakes occur there. The next
most seismic region (5 - 6 % of earthquakes) is the Alpide belt.</p>
</dd>
<dt id="term-RMS">RMS<a class="headerlink" href="#term-RMS" title="Permalink to this term"></a></dt><dd><p>Abbreviation for <a class="reference internal" href="#term-root-mean-square-RMS"><span class="xref std std-term">root mean square</span></a></p>
</dd>
<dt id="term-root-mean-square-RMS">root mean square (RMS)<a class="headerlink" href="#term-root-mean-square-RMS" title="Permalink to this term"></a></dt><dd><p>Also referred to as <a class="reference internal" href="#term-RMS"><span class="xref std std-term">RMS</span></a>. A statistical measure of the magnitude of a varying quantity defined as</p>
<div class="math">
<p><img src="../_images/math/2f6a630b284c6a5d80008de8acea2f431a388d2c.png" alt="RMS = \sqrt{\frac{{x_1}^2 + {x_2}^2 + {x_3}^2 + ... + {x_n}^2}{N}}"/></p>
</div><p>for the time series with the N elements x<sub>1</sub> to x<sub>n</sub>.</p>
</dd>
<dt id="term-rupture-front">rupture front<a class="headerlink" href="#term-rupture-front" title="Permalink to this term"></a></dt><dd><p>The instantaneous boundary between the slipping and locked parts of a fault during
an earthquake. A rupture propagating in one direction on the fault is referred to
as unilateral. A rupture may radiate outward in a circular manner or it may radiate
towards the two ends of the fault from an interior point, behavior referred to as
bilateral.</p>
</dd>
<dt id="term-rupture-velocity">rupture velocity<a class="headerlink" href="#term-rupture-velocity" title="Permalink to this term"></a></dt><dd><p>The speed at which a rupture front moves across the surface of the fault during
an earthquake.</p>
</dd>
<dt id="term-SCML">SCML<a class="headerlink" href="#term-SCML" title="Permalink to this term"></a></dt><dd><p><a class="reference internal" href="#term-SeisComP"><span class="xref std std-term">SeisComP</span></a> Markup Language. SCML is a flavor of <a class="reference external" href="https://quake.ethz.ch/quakeml/">QuakeML</a> and is used by <cite>SeisComP</cite> and by
products of <a class="reference internal" href="#term-gempa-GmbH"><span class="xref std std-term">gempa GmbH</span></a> for exchange. For details read the
<a class="reference external" href="https://geofon.gfz-potsdam.de/_uml/">UML diagram</a>.</p>
</dd>
<dt id="term-SDS">SDS<a class="headerlink" href="#term-SDS" title="Permalink to this term"></a></dt><dd><p><cite>SeisComP</cite> Data Structure which is used for archiving waveform data. Below the
base directory of the archive the SDS has the structure:</p>
<div class="highlight-sh notranslate"><div class="highlight"><pre><span></span>archive
<span class="w"> </span>+<span class="w"> </span>year
<span class="w"> </span>+<span class="w"> </span>network<span class="w"> </span>code
<span class="w"> </span>+<span class="w"> </span>station<span class="w"> </span>code
<span class="w"> </span>+<span class="w"> </span>channel<span class="w"> </span>code
<span class="w"> </span>+<span class="w"> </span>one<span class="w"> </span>file<span class="w"> </span>per<span class="w"> </span>day<span class="w"> </span>and<span class="w"> </span>location,<span class="w"> </span>e.g.<span class="w"> </span>NET.STA.LOC.CHAN.D.YEAR.DOY
</pre></div>
</div>
</dd>
<dt id="term-SED">SED<a class="headerlink" href="#term-SED" title="Permalink to this term"></a></dt><dd><p>Specific Energy Density</p>
</dd>
<dt id="term-SeedLink">SeedLink<a class="headerlink" href="#term-SeedLink" title="Permalink to this term"></a></dt><dd><p>SeedLink <span id="id12">[<a class="reference internal" href="references.html#id253" title="seedlink. Real-time waveform server. URL: https://docs.gempa.de/seiscomp/current/apps/seedlink.html.">30</a>]</span> is a
real-time data acquisition protocol and a client-server software that
implements this protocol</p>
</dd>
<dt id="term-SeisComP">SeisComP<a class="headerlink" href="#term-SeisComP" title="Permalink to this term"></a></dt><dd><p>SeisComP is likely the most widely distributed software package for
seismological data acquisition and real-time data exchange over internet.
Its data transmission protocol SeedLink became a de facto world standard.
The first version of SeisComP was developed for the <a class="reference external" href="http://geofon.gfz-potsdam.de/geofon/">GEOFON</a> network and further extended
within the MEREDIAN project under the lead of <a class="reference external" href="http://geofon.gfz-potsdam.de/geofon/">GEOFON</a>/<a class="reference external" href="http://www.gfz-potsdam.de/">GFZ</a> Potsdam and <a class="reference external" href="http://www.orfeus-eu.org/">ORFEUS</a>. Originally SeisComP was designed as a high
standard fully automatic data acquisition and (near-)real-time data
processing tool including quality control, event detection and location as
well as dissemination of event alerts. In the context of the <a class="reference external" href="http://www.gitews.de/">GITEWS</a> project (German Indian Ocean Tsunami Early
Warning System) additional functionality were implemented to fulfill the
requirements of 24/7 early warning control centers. Major changes in the
architecture of SeisComP were necessary and many new features result in
the upgrade of SeisComP to version 3. Important SeisComP releases are
shown below. A first prototype of <a class="reference internal" href="#term-SeisComP3"><span class="xref std std-term">SeisComP3</span></a> developed by the
GITEWS/GEOFON development group was released in May 2007.</p>
</dd>
<dt id="term-SeisComP3">SeisComP3<a class="headerlink" href="#term-SeisComP3" title="Permalink to this term"></a></dt><dd><p>A previous version of <a class="reference internal" href="#term-SeisComP"><span class="xref std std-term">SeisComP</span></a>.</p>
</dd>
<dt id="term-seismic-array">seismic array<a class="headerlink" href="#term-seismic-array" title="Permalink to this term"></a></dt><dd><p>An ordered arrangement of seismometers with central data acquisition specially
designed to analyze seismic signal based on coherent phases. A seismic array
differs from a local network of seismic stations mainly by the techniques
used for data analysis. Often, a seismic array are referred to as <a class="reference internal" href="#term-array"><span class="xref std std-term">array</span></a>.</p>
</dd>
<dt id="term-seismic-gap">seismic gap<a class="headerlink" href="#term-seismic-gap" title="Permalink to this term"></a></dt><dd><p>A section of a fault that has produced earthquakes in the past but is now quiet.
For some seismic gaps, no earthquakes have been observed historically, but it is
believed (based on some other methods, such as plate-motion information, strain
measurements or geological observations) that the fault segment is capable of
producing earthquakes. A long-term seismic gap may give hint to the most probable
location of a strong earthquake in the future.</p>
</dd>
<dt id="term-seismic-moment-M0">seismic moment (M<sub>0</sub>)<a class="headerlink" href="#term-seismic-moment-M0" title="Permalink to this term"></a></dt><dd><p>The seismic moment is defined as</p>
<div class="math">
<p><img src="../_images/math/8f1708ea69c95606206a9c9491a7664a7d3ebcfc.png" alt="M_0 = \mu D A"/></p>
</div><p>with μ as rigidity of the rock at the fault, D as averaged displacement on the
fault and A as fault surface area. For pure shear sources, M<sub>0</sub> equals
the <a class="reference internal" href="#term-total-seismic-moment-MT"><span class="xref std std-term">total seismic moment (MT)</span></a>.
The seismic moment can be related to the released seismic energy ES that is
proportional to the stress drop Δσ:</p>
<div class="math">
<p><img src="../_images/math/045405e3ed4451fb8c73dfa60cf0db9d9c09b15e.png" alt="E_S \approx 0.5 \Delta\sigma D A"/></p>
</div><p>Rearranging both equations yields to:</p>
<div class="math">
<p><img src="../_images/math/bfb9920a001f8f2088e3444b21712bc8ce7eea27.png" alt="E_S \approx \frac{\Delta\sigma}{2\mu} M_0"/></p>
</div><p>M<sub>0</sub> can be determined by the asymptote of the amplitude spectrum at
frequency = 0.
A common technique for determination of the seismic moment M<sub>0</sub> is the
moment tensor inversion. Assuming reasonable values for the rigidity of the
rock (3-6 x 104 MPa in crust and upper mantle) and the stress drop (2-6 MPa)
the seismic moment can be related to the surface wave magnitude Ms by the
empirical relationship found by <span id="id14">Gutenberg and Richter [<a class="reference internal" href="references.html#id36" title="B. Gutenberg and C.F. Richter. Magnitude and Energy of Earthquakes. Annals of Geophysics, 9(1):1 - 15, 1956. URL: https://resolver.caltech.edu/CaltechAUTHORS:20140130-105324849, doi:10.4401/ag-5590.">43</a>]</span> (units in cgs):</p>
<div class="math">
<p><img src="../_images/math/d7e59ce0e8d9250bee9b829d4a243edee8473113.png" alt="\log E_S = 11.8 + 1.5 Ms
\log M_0 = 1.5 Ms + 16.1"/></p>
</div></dd>
<dt id="term-seismic-network">seismic network<a class="headerlink" href="#term-seismic-network" title="Permalink to this term"></a></dt><dd><p>Group of seismic stations that are deployed as single stations or arrays.</p>
</dd>
<dt id="term-seismic-ray">seismic ray<a class="headerlink" href="#term-seismic-ray" title="Permalink to this term"></a></dt><dd><p>Vector perpendicular to the wave front pointing into the direction of wave
propagation and marking behind it the “ray trace”. The propagation of seismic
waves can be easily modelled as the propagation of seismic rays following
Snells Law. This assumption is a reasonable approximation for high frequency waves.</p>
</dd>
<dt id="term-seismic-signal">seismic signal<a class="headerlink" href="#term-seismic-signal" title="Permalink to this term"></a></dt><dd><p>A coherent transient waveform radiated from a definite, localized seismic source
that is usually considered as an useful signal for the location of the source,
the analysis of the source process and/or of the propagation medium (in contrast to noise).</p>
</dd>
<dt id="term-seismic-source">seismic source<a class="headerlink" href="#term-seismic-source" title="Permalink to this term"></a></dt><dd><p>A localized area or volume generating coherent, usually transient seismic waveforms,
such as an earthquake, explosion, vibrator etc.</p>
</dd>
<dt id="term-semblance">semblance<a class="headerlink" href="#term-semblance" title="Permalink to this term"></a></dt><dd><p>Normalized <a class="reference internal" href="#term-beam-power"><span class="xref std std-term">beam power</span></a>.</p>
</dd>
<dt id="term-signal-to-noise-ratio">signal-to-noise ratio<a class="headerlink" href="#term-signal-to-noise-ratio" title="Permalink to this term"></a></dt><dd><p>The comparison between the amplitude of the seismic signal and the amplitude of
the noise; abbreviated as <a class="reference internal" href="#term-SNR"><span class="xref std std-term">SNR</span></a>.</p>
</dd>
<dt id="term-slab">slab<a class="headerlink" href="#term-slab" title="Permalink to this term"></a></dt><dd><p>Usually, the part of the <a class="reference internal" href="#term-lithosphere"><span class="xref std std-term">lithospheric</span></a>
plate that is underthrusting in a subduction zone and is
consumed by the Earths mantle is called slab.</p>
</dd>
<dt id="term-slab-pull">slab pull<a class="headerlink" href="#term-slab-pull" title="Permalink to this term"></a></dt><dd><p>The force of gravity causing the cooler and denser oceanic <a class="reference internal" href="#term-slab"><span class="xref std std-term">slab</span></a> to sink
into the
hotter and less dense mantle material. The downdip component of this force leads
to downdip extensional stress in the slab and may produce earthquakes within the
subducted slab. Slab pull may also contribute to stress on the subduction thrust
fault if the fault is locked.</p>
</dd>
<dt id="term-slip">slip<a class="headerlink" href="#term-slip" title="Permalink to this term"></a></dt><dd><p>The relative displacement of formerly adjacent points on opposite sides of a fault.</p>
</dd>
<dt id="term-slip-model">slip model<a class="headerlink" href="#term-slip-model" title="Permalink to this term"></a></dt><dd><p>A kinematic model that describes the amount, distribution, and timing of a slip
associated with an earthquake.</p>
</dd>
<dt id="term-slip-rate">slip rate<a class="headerlink" href="#term-slip-rate" title="Permalink to this term"></a></dt><dd><p>How fast the two sides of a fault are slipping relative to one another, as
derived from seismic records in case of an earthquake or determined, as a
long-term average, from geodetic measurements, from offset man-made structures,
or from offset geologic features whose age can be estimated. It is measured
parallel to the predominant slip direction or estimated from the vertical or
horizontal offset of geologic markers.</p>
</dd>
<dt id="term-slowness">slowness<a class="headerlink" href="#term-slowness" title="Permalink to this term"></a></dt><dd><p>The inverse of velocity, given in the unit seconds/degree or s/km; a large
slowness corresponds to a low velocity.</p>
</dd>
<dt id="term-SNR">SNR<a class="headerlink" href="#term-SNR" title="Permalink to this term"></a></dt><dd><p>Abbreviation for <a class="reference internal" href="#term-signal-to-noise-ratio"><span class="xref std std-term">signal-to-noise ratio</span></a>.</p>
</dd>
<dt id="term-source-depth">source depth<a class="headerlink" href="#term-source-depth" title="Permalink to this term"></a></dt><dd><p>Location of an earthquake below the Earths surface. Earthquakes can occur
between the surface and depths of about 700 km. Usually three classes of
earthquakes are separated according to the depth: Shallow earthquakes occur
in the depth range of 0 to 70 km; intermediate earthquakes between 70 and 300km
depth; and deep earthquakes between 300 and 700 km depth. Earthquakes at large
depths occur much less frequent than shallow earthquakes. Additionally, deep
earthquakes excite small surface waves compared to the body waves and relatively
simple P and S waveforms with more impulsive onsets. A more reliable way to
determine the depth of an earthquake is to identify depth phases (e.g. pP, sP)
in the waveforms. At stations with large distance to the epicenter the pP wave
follows the direct P wave by a time interval that slightly increases with distance
but rapidly with depth. The depth can be derived from this time interval by using
<a class="reference internal" href="#term-travel-time-curve"><span class="xref std std-term">travel-time curves</span></a>.</p>
</dd>
<dt id="term-source-time-function">source time function<a class="headerlink" href="#term-source-time-function" title="Permalink to this term"></a></dt><dd><p>The source time function describes the ground motion generated at the fault over
time. The function is predicted by a theoretical model.</p>
</dd>
<dt id="term-Spooler">Spooler<a class="headerlink" href="#term-Spooler" title="Permalink to this term"></a></dt><dd><p>Application which watches a directory for new bulletins and performs the
final and service specific dissemination operation. This may involve
talking to modem (for fax, SMS), connecting to a SMTP server (email) or
rendering a Web page.</p>
</dd>
<dt id="term-station">station<a class="headerlink" href="#term-station" title="Permalink to this term"></a></dt><dd><p>Site of measurement typically consisting of one or more sensors and one or
more dataloggers.</p>
</dd>
<dt id="term-station-magnitude">station magnitude<a class="headerlink" href="#term-station-magnitude" title="Permalink to this term"></a></dt><dd><ol class="arabic simple">
<li><p>The station magnitude is the magnitude value based on the amplitude measurements of a single station.
Due to radiation pattern, site and path effects and the calibration of the station the station magnitudes
of one event can scatter significantly.</p></li>
<li><p>QuakeML object</p></li>
</ol>
</dd>
<dt id="term-stick-slip">stick-slip<a class="headerlink" href="#term-stick-slip" title="Permalink to this term"></a></dt><dd><p>The rapid displacement that occurs between two sides of a fault when the shear stress
on the fault exceeds the frictional stress. Also a jerky, sliding type of motion
associated with fault movement in laboratory experiments. It may be a mechanism
in shallow earthquakes. Stick -slip displacement on a fault radiates energy in the
form of seismic waves.</p>
</dd>
<dt id="term-stress-drop">stress drop<a class="headerlink" href="#term-stress-drop" title="Permalink to this term"></a></dt><dd><p>The difference between the stress across a fault before and after an earthquake.
A parameter in many models of the earthquake source that affects the level of
high-frequency shaking radiated by the earthquake. Commonly stated in units termed
bars or megapascals (1 bar equals 1 kg/cm², and 1 megapascal equals 10 bars).</p>
</dd>
<dt id="term-T">T<a class="headerlink" href="#term-T" title="Permalink to this term"></a></dt><dd><p>period, time duration</p>
</dd>
<dt id="term-takeoff-angle">takeoff angle<a class="headerlink" href="#term-takeoff-angle" title="Permalink to this term"></a></dt><dd><p>The angle that a seismic ray makes with a downward vertical axis through the
source. Rays with takeoff angles less than 90° are labeled with capital letters
like P or S. If the takeoff angle is greater than 90° the ray is upgoing and is
labeled with lowercase letters (p or s). Such rays can be reflected at the
surface near the epicenter forming a depth phase (see <a class="reference internal" href="#term-pP-phase"><span class="xref std std-term">pP phase</span></a> or <a class="reference internal" href="#term-sP-phase"><span class="xref std std-term">sP phase</span></a>).</p>
</dd>
<dt id="term-teleseismic">teleseismic<a class="headerlink" href="#term-teleseismic" title="Permalink to this term"></a></dt><dd><p>Pertaining to a seismic source at distances greater than about 2000 km from the
measurement site.</p>
</dd>
<dt id="term-theoretical-onset">theoretical onset<a class="headerlink" href="#term-theoretical-onset" title="Permalink to this term"></a></dt><dd><p>The point where an arrival is expected to appear on a seismic record, based
on the known location and depth of the seismic source and according to a velocity
model.</p>
</dd>
<dt id="term-time-domain">time domain<a class="headerlink" href="#term-time-domain" title="Permalink to this term"></a></dt><dd><p>A seismic record is usually presented in the time domain, i.e., as a display of
varying amplitudes of (filtered) ground motion as a function of time (in contrast
to the equivalent representation in the frequency domain) (see also Fourier analysis).</p>
</dd>
<dt id="term-Tp">Tp<a class="headerlink" href="#term-Tp" title="Permalink to this term"></a></dt><dd><p>predominant period</p>
</dd>
<dt id="term-Tm">Tm<a class="headerlink" href="#term-Tm" title="Permalink to this term"></a></dt><dd><p>mean period</p>
</dd>
<dt id="term-total-seismic-moment-MT">total seismic moment (MT)<a class="headerlink" href="#term-total-seismic-moment-MT" title="Permalink to this term"></a></dt><dd><p>A measure of the strength of the full <a class="reference internal" href="#term-moment-tensor"><span class="xref std std-term">moment tensor</span></a>:</p>
<div class="math">
<p><img src="../_images/math/1712005c894ef6c6244697d1123cc2c090368cb3.png" alt="M_T = \sqrt{\sum_{ij}M_{ij}M_{ij}/2}"/></p>
</div><p>For pure shear sources M<sub>T</sub> equals <a class="reference internal" href="#term-seismic-moment-M0"><span class="xref std std-term">seismic moment (M0)</span></a>.</p>
</dd>
<dt id="term-transfer-function">transfer function<a class="headerlink" href="#term-transfer-function" title="Permalink to this term"></a></dt><dd><p>The transfer function of a seismic sensor-recorder system (or of the Earth
medium through which seismic waves propagate) describes the frequency-dependent
amplification, damping and phase distortion of seismic signals by a specific
sensor-recorder (or medium). The modulus (real term = absolute value) of the
transfer function is termed the frequency response function or magnification
curve, e.g. of a seismograph.</p>
</dd>
<dt id="term-travel-time">travel time<a class="headerlink" href="#term-travel-time" title="Permalink to this term"></a></dt><dd><p>The time required for a wave traveling from its source to a point of observation.</p>
</dd>
<dt id="term-travel-time-curve">travel-time curve<a class="headerlink" href="#term-travel-time-curve" title="Permalink to this term"></a></dt><dd><p>A graph of arrival times, commonly of direct as well as multiply reflected and
converted <a class="reference internal" href="#term-P-wave"><span class="xref std std-term">P</span></a> or <a class="reference internal" href="#term-S-wave"><span class="xref std std-term">S waves</span></a>, recorded at different
points as a function of distance
from the seismic source. Seismic velocities within the Earth can be computed
from the slopes of the resulting curves.</p>
</dd>
<dt id="term-XXL-event">XXL event<a class="headerlink" href="#term-XXL-event" title="Permalink to this term"></a></dt><dd><p>An event based on <a class="reference internal" href="#term-XXL-pick"><span class="xref std std-term">XXL picks</span></a>.</p>
</dd>
<dt id="term-XXL-pick">XXL pick<a class="headerlink" href="#term-XXL-pick" title="Permalink to this term"></a></dt><dd><p>Picks that have extraordinarily large amplitudes and large <a class="reference internal" href="#term-SNR"><span class="xref std std-term">SNR</span></a> and
that lie within a relatively small region.</p>
</dd>
<dt id="term-vespagram">vespagram<a class="headerlink" href="#term-vespagram" title="Permalink to this term"></a></dt><dd><p>Vespagrams are diagrams of <a class="reference internal" href="#term-beam"><span class="xref std std-term">beam</span></a> traces over time typically formed
for a particular <a class="reference internal" href="#term-azimuth"><span class="xref std std-term">azimuth</span></a> (or <a class="reference internal" href="#term-backazimuth"><span class="xref std std-term">backazimuth</span></a>) and for
ranges of <a class="reference internal" href="#term-slowness"><span class="xref std std-term">slowness</span></a> (slowness vespagram). When the slowness
is kept constant and the backazimuth is varied the term backazimuth
vespagram is used.</p>
</dd>
<dt id="term-Wadati-Benioff-zone">Wadati-Benioff zone<a class="headerlink" href="#term-Wadati-Benioff-zone" title="Permalink to this term"></a></dt><dd><p>A dipping planar (flat) zone of earthquakes that is produced by the interaction
of a downgoing oceanic crustal plate with a continental plate. These earthquakes
can be produced by slip along the subduction thrust fault (thrust interface between
the continental and the oceanic plate) or by slip on faults within the downgoing
plate as a result of bending and extension as the plate is pulled into the mantle.
Slip may also initiate between adjacent segments of downgoing plates. Wadati-Benioff
zones are usually well-developed along the trenches of the Circum-Pacific belt,
dipping towards the continents.</p>
</dd>
<dt id="term-wave-number">wave number<a class="headerlink" href="#term-wave-number" title="Permalink to this term"></a></dt><dd><p>Number of cycles of a repeating signal per unit length, typically per meter of kilometer.</p>
</dd>
<dt id="term-P-wave">P wave<a class="headerlink" href="#term-P-wave" title="Permalink to this term"></a></dt><dd><p>P (primary) waves are compressional waves involving volumetric variations in the
media. The sense of particle motion is linear and parallel to the propagation
direction. P waves are body waves that traverse the interior of a body/Earth and
can propagate in fluids.</p>
<p>The general nomenclature for P waves: At local and
regional distances a special nomenclature is used to describe the travel path of
the first P and S arrivals. Pg, Pb/P* and Pn phases are separated. Pg is the direct
P wave arriving first in distances less than around 100 km. Pn is the head wave
along the Moho arriving first at larger distances than 100 km (depending on the
crustal thickness). Pn has usually smaller amplitudes than Pg. Pb or P* is the
rarely observed head wave travelling along the midcrustal velocity discontinuity.
The general nomenclature of P waves entitles reflections at the topside of boundaries
with lowercase letters (m Moho reflection; c - CMB reflection; i - inner core-outer
core boundary reflection), e.g. PmP is a reflected P wave at the Moho. Reflections
at the bottom side of boundaries get no additional letter, e.g. PP is a reflected
P wave at the Earths surface. Refracted rays get capital letters (K - through
the outer core; I - through the inner core), e.g. PKIKP is a P wave traversing
the crust/mantle, the outer core, the inner core, again the outer core and again
the mantle/crust.</p>
</dd>
<dt id="term-S-wave">S wave<a class="headerlink" href="#term-S-wave" title="Permalink to this term"></a></dt><dd><p>S (secondary) waves are shear waves without any volumetric variation in the media.
The sense of particle motion is perpendicular to the propagation direction. S waves
are body waves that traverse the interior of a body but can not propagate in fluids.</p>
<p>Analog to the P arrivals Sg, Sb/S<sup>*</sup> and Sn arrivals are distinguished in local
and regional distances. The general nomenclature of S waves is analog to the P waves.
The reflections at the topside of boundaries have lowercase letters (m - Moho
reflection; c - CMB reflection), e.g. SmS is a reflected S wave at the Moho.
Reflections at the bottom side of boundaries get no additional letter, e.g. SS is a
reflected S wave at the Earths surface. Refracted rays get capital letters (J - through
the inner core), e.g. SKJKS is a S wave traversing the crust/mantle, the outer core
as a <a class="reference internal" href="#term-P-wave"><span class="xref std std-term">P wave</span></a>, the inner core as a <a class="reference internal" href="#term-S-wave"><span class="xref std std-term">S wave</span></a>, again the outer core as a P wave and again
the mantle/crust as S wave. S waves can not travel through the outer core because
the outer core consists of a fluid.</p>
</dd>
<dt id="term-surface-wave">surface wave<a class="headerlink" href="#term-surface-wave" title="Permalink to this term"></a></dt><dd><p>Surface waves are seismic waves observed only at the free surface of the media.
Two types of surface waves are distinguished: <a class="reference internal" href="#term-Love-wave"><span class="xref std std-term">Love waves</span></a> (L)
and <a class="reference internal" href="#term-Rayleigh-wave"><span class="xref std std-term">Rayleigh waves</span></a> (R).
Both result from the interaction of P and S waves near the free surface.</p>
</dd>
<dt id="term-waveform-data">waveform (data)<a class="headerlink" href="#term-waveform-data" title="Permalink to this term"></a></dt><dd><p>The complete analog or sufficiently dense sampled digital representation of a
continuous wave group (e.g., of a seismic phase) or of a whole wave train
(seismogram). Accordingly, waveform data allow to reconstruct and analyze the
whole seismic phase or earthquake record both in the time and frequency domain
whereas parameter data describe the signal only by a very limited number of more
or less representative measurements such as onset time, maximum signal amplitude
and related period.</p>
</dd>
<dt id="term-waveformID">waveformID<a class="headerlink" href="#term-waveformID" title="Permalink to this term"></a></dt><dd><p>Attribute of the QuakeML objects Pick, !StationAmplitude and !StationMagnitude
describing the source of the underlying waveform source. The WaveformID contains
information about the !NetworkCode, !StationCode, !LocationCode and !ChannelCode</p>
</dd>
<dt id="term-wave-front">wave front<a class="headerlink" href="#term-wave-front" title="Permalink to this term"></a></dt><dd><p>The surface formed by all elements of a propagating wave, which swing in phase;
the wave front is perpendicular to the seismic rays, which are oriented in
direction of wave propagation.</p>
</dd>
<dt id="term-wavelength">wavelength<a class="headerlink" href="#term-wavelength" title="Permalink to this term"></a></dt><dd><p>The distance between successive points of equal amplitude and phase on a
wave (for example, crest to crest or trough to trough).</p>
</dd>
<dt id="term-weight">weight<a class="headerlink" href="#term-weight" title="Permalink to this term"></a></dt><dd><p>Attribute of the QuakeML objects Arrival and !MagnitudeReferences defining the
effect of the referenced object (e.g. Pick).</p>
</dd>
<dt id="term-Wood-Anderson-seismometer">Wood-Anderson seismometer<a class="headerlink" href="#term-Wood-Anderson-seismometer" title="Permalink to this term"></a></dt><dd><p>Torsion seismometer recording horizontal displacement
<a class="reference internal" href="#term-amplitude"><span class="xref std std-term">amplitudes</span></a> described in <span id="id15">Richter [<a class="reference internal" href="references.html#id62" title="C.F. Richter. An instrumental earthquake magnitude scale. Bull. Seismol. Soc. Am., 1:1 - 32, 1935. URL: https://resolver.caltech.edu/CaltechAUTHORS:20140804-143558638, doi:10.1785/BSSA0250010001.">57</a>]</span> and
<span id="id16">Uhrhammer and Collins [<a class="reference internal" href="references.html#id81" title="R.A. Uhrhammer and E.R. Collins. Synthesis of Wood-Anderson seismograms from broadband digital records. Bull. Seismol. Soc. Am., 80(3):702716, 1990. doi:10.1785/BSSA0800030702.">64</a>]</span>. Simulation of the Wood-Anderson seismometer is
used for measuring amplitudes for selected <a class="reference internal" href="#term-magnitude"><span class="xref std std-term">magnitudes</span></a>.
SeisComP3 and SeisComP in versions 4 and 5 have considered Wood-Anderson
instrument parameters originally published by <span id="id17">Richter [<a class="reference internal" href="references.html#id62" title="C.F. Richter. An instrumental earthquake magnitude scale. Bull. Seismol. Soc. Am., 1:1 - 32, 1935. URL: https://resolver.caltech.edu/CaltechAUTHORS:20140804-143558638, doi:10.1785/BSSA0250010001.">57</a>]</span> with
gain = 2800, T0 = 0.8 s, h = 0.8. However, updated parameters where
published by <span id="id18">Uhrhammer and Collins [<a class="reference internal" href="references.html#id81" title="R.A. Uhrhammer and E.R. Collins. Synthesis of Wood-Anderson seismograms from broadband digital records. Bull. Seismol. Soc. Am., 80(3):702716, 1990. doi:10.1785/BSSA0800030702.">64</a>]</span> with gain = 2080, T0 = 0.8 s,
h = 0.7. These values were part of the IASPEI Magnitude Working Group
recommendations of 2011 September 9 and therefore apply by default in later
versions of SeisComP. With the original set of values
<span id="id19">[<a class="reference internal" href="references.html#id62" title="C.F. Richter. An instrumental earthquake magnitude scale. Bull. Seismol. Soc. Am., 1:1 - 32, 1935. URL: https://resolver.caltech.edu/CaltechAUTHORS:20140804-143558638, doi:10.1785/BSSA0250010001.">57</a>]</span>, magnitudes are systematically overestimated by 0.13.
Wood-Anderson seismometers can be simulated by filtering waveforms with
<a class="reference internal" href="filter-grammar.html#WA" title="WA"><code class="xref py py-func docutils literal notranslate"><span class="pre">WA()</span></code></a>.</p>
</dd>
<dt id="term-WWSSN_SP">WWSSN_SP<a class="headerlink" href="#term-WWSSN_SP" title="Permalink to this term"></a></dt><dd><p>Short period seismograph with a dominant period of 1 s of the World-Wide
Standard Seismograph Network (WWSSN). WWSSN_SP instruments can be simulated
by filtering waveforms with <a class="reference internal" href="filter-grammar.html#WWSSN_SP" title="WWSSN_SP"><code class="xref py py-func docutils literal notranslate"><span class="pre">WWSSN_SP()</span></code></a>.</p>
</dd>
<dt id="term-WWSSN_LP">WWSSN_LP<a class="headerlink" href="#term-WWSSN_LP" title="Permalink to this term"></a></dt><dd><p>Long period seismograph with a dominant period of 20 s of the World-Wide
Standard Seismograph Network (WWSSN). WWSSN_LP instruments can be simulated
by filtering waveforms with <a class="reference internal" href="filter-grammar.html#WWSSN_LP" title="WWSSN_LP"><code class="xref py py-func docutils literal notranslate"><span class="pre">WWSSN_LP()</span></code></a>.</p>
</dd>
<dt id="term-XML">XML<a class="headerlink" href="#term-XML" title="Permalink to this term"></a></dt><dd><p>Extensible Markup Language a version of which is <a class="reference internal" href="#term-SCML"><span class="xref std std-term">SCML</span></a>.</p>
</dd>
</dl>
<section id="distance-terms">
<h3>Distance terms<a class="headerlink" href="#distance-terms" title="Permalink to this heading"></a></h3>
<dl class="simple glossary">
<dt id="term-distance-epicentral">distance, epicentral<a class="headerlink" href="#term-distance-epicentral" title="Permalink to this term"></a></dt><dd><p>The epicentral distance is defined as the shortest distance from a seismic
station or any other site to the epicentre of the seismic event.</p>
</dd>
<dt id="term-distance-hypocentral">distance, hypocentral<a class="headerlink" href="#term-distance-hypocentral" title="Permalink to this term"></a></dt><dd><p>The hypocentral distance is defined as the shortest distance from a
seismic station or any other site to the hypocentre of the seismic event.</p>
</dd>
</dl>
</section>
</section>
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