「detector」の共起表現(1語左が「the」)

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共起表現

「detector」の共起表現一覧(1語左が「the」)

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Specify the	detector geometry.
Otherwise the	detector might be damaged.
Roughly spherical, the	detector measures 30 feet across.
The outermost layer of the	detector detects muons.
the satellite made the interpretation of the	detector data very difficult.
As a charged particle travels through the	detector, it ionizes the gas between the plates.
In a second phase (end of 2007), the	detector is planned to be moved underground.
rcentage of the fluorescence picked up by the	detector is also dependent upon the system.
On passing through the	detector gas, a particle will produce primary ionizati
By contrast, if the	detector sees photons emitted directly from a glowing
ition of endcaps of similar construction, the	detector covered 98% of the solid angle around the int
After its decommissioning at SLAC, the	detector was carried to DESY, where it was used for b-
o discriminate against particles entering the	detector from below.
upersymmetric particle, LSP (which leaves the	detector unseen).
The intensity of the light hitting the	detector depends on the relative positions of the two
ten built underground in order to isolate the	detector from cosmic rays and other background radiati
is nearing the levels where theoretically the	detector should start to detect dark matter.
Even though the	detector operated only during a few months in the summ
The LEGRI system included the	Detector Unit, Mask Unit, Power Supply, Digital Proces
The polarized radiation focused onto the	detector is doubly modulated, both by the PEM and by t
These two components interfere in the	detector and produce signals, which permit the detecti
band of light initially traveling toward the	detector, has been effectively scattered in other dire
of a defined energy are backscattered to the	detector if they collide with an atomic nucleus.
ved signal to a level sufficient to drive the	detector stage.
The bubble development in the	detector is accompanied by an acoustic shock wave that
, if no higher energy particles penetrate the	detector walls, the SST-Foil should only measure elect
Since the ray cones approaching the	detector surface have the same angle of incidence and
s VD slowly recovers to Va, and therefore the	detector is ready to be ignited again.
th a so-called makeup gas flowing through the	detector chamber.
d by this low voltage and will only reach the	detector if their direction of travel takes them to it
sufficient energy such that it arrives at the	detector at the same time as the red ion.
ill then drift through the flight tube to the	detector in the same time.
The scattered gamma rays reaching the	detector, at the fixed station from the source, are co
The order of migration seen by the	detector is shown in figure 3: small multiply charged
ting the spatial information contained in the	detector signal we can more accurately localize the γ-
The first part of NT-200, the	detector NT-36 with 36 optical modules (OMs) at 3 shor
/z but different kinetic energy arrive at the	detector at the same time.
gain is how the amount of signal given by the	detector varies as a function of the amount of light (
rent is the amount of signal given out by the	detector when there is no incident light (hence dark f
sed for fine adjustment of the sample and the	detector positions.
The use of a mass spectrometer as the	detector in gas chromatography was developed during th
The name of the	detector is a playful pun, which was bestowed upon it
aser intensity, the quantum efficiency of the	detector and the full scattering volume and solid angl
es are necessary: an underground site for the	detector, to limit the effect of the seismic noise, an
Deployment and connection of the	detector are performed in cooperation with the French
era phones, because the low resolution of the	detector allows a loose focusing on the CCD without no
can undergo a phase transition at a time, the	detector can stay active for much longer periods than
flicker frequency of a fire (1 to 20 Hz) the	detector is made less sensitive to false alarms, cause
of SSNTDs is that charged particles break the	detector within nanometers down the path in such a way
and positron created were measured within the	detector volume,and the axis of the V of the two emerg
25 (GX5-1), but the spatial resolution of the	detector was insufficient to resolve Sgr X-5 from the
Case described the	detector material as consisting of thallium, oxygen an
eld that the ions recombine after passing the	detector to reform their original molecules, however o
oherent superposition of emitted light on the	detector is possible.
ation of intensity from any Debye cone at the	detector provides order(s) of magnitude increase in in
ich case the (nearly) steady component of the	detector output is a good measure of the instantaneous
order to filter out the common events so the	detector is not overwhelmed, the electrons must pass t
e overall signal production efficiency of the	detector, however, also depends on the quantum efficie
by the linear stage and appear finally to the	detector as if it were a sideband of the carrier, it i
er signal is given when the sample enters the	detector because the oxidized carbons are not ionized

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「detector」の共起表現一覧(1語左が「the」)