「Electrons」の共起表現一覧(1語右で並び替え)
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R theory because xenon has two lone pairs of | electrons above and below the plane of the molecule. |
969, is considered to be bremsstrahlung from | electrons accelerated in two stages in the solar atmos |
Diffraction occurs because the wavelength of | electrons accelerated by a potential of a few thousand |
miconductor must have enough energy to raise | electrons across the band gap, or to excite the impuri |
s are able to generate excitons by promoting | electrons across the band gap. |
r as the light absorption is due to exciting | electrons across the band gap). |
electrons, alpha particles, or hydrogen ions | |
hus the B2H2 ring is held together with four | electrons, an example of 3-center-2-electron bonding. |
that is, all stoichiometric combinations of | electrons and atomic nuclei, in all possible topology |
A negative trion consists of two | electrons and one hole and a positive trion consists o |
xygen, water is not created and in its place | electrons and hydrogen ions are formed. |
e accelerators use electric fields to propel | electrons and their antiparticles to high energies. |
collectors to recycle kinetic energy of the | electrons and therefore the secondary winding of the p |
This article is about the mobility for | electrons and holes in metals and semiconductors. |
ascorbate acts as a reducing agent, donating | electrons and preventing oxidation to keep iron and co |
ering from the right), producing x-rays, hot | electrons, and an ion beam, which cannot be seen direc |
It began running in 1972, colliding | electrons and positrons with an energy of 3 GeV. |
The | electrons and holes react with the surrounding water v |
The nitrogen atom has only 6 valence | electrons and is therefore considered an electrophile. |
of the neutral atom, the mass of the missing | electrons and their binding energies have to be added |
orbitals and orbital energies for the α spin | electrons and a set of molecular orbitals and orbital |
e α phase bonds are mediated by the 5f shell | electrons, and can be disrupted by increased temperatu |
2's high hardness: a high density of valence | electrons, and an abundance of short covalent bonds. |
such as a semiconductor, the number of free | electrons and electron holes changes and raises its el |
stripped of | electrons and concentrated into a 2 MW proton beam of |
up of a hot, interacting plasma of photons, | electrons, and baryons. |
of fixed energy into which can be placed two | electrons and no more. |
k current is due to the random generation of | electrons and holes within the depletion region of the |
the positive plate, they then give up their | electrons and become positively charged like the plate |
It contains no unpaired | electrons and reacts readily with water disproportiona |
remnants into leptons (such as positrons and | electrons) and photons. |
ATIC cannot distinguish between | electrons and positrons, so it is possible that the tw |
first time how much energy it takes to move | electrons and protons in a metal-protein complex |
Hence, there is a constant flow of | electrons and associated hydrogens from water for the |
interactions is set by the number density of | electrons and positrons, the averaged product of the c |
model the interaction between the conduction | electrons and the ions in a crystalline solid. |
ectra, and angular distribution of energetic | electrons and protons in interplanetary space and near |
to produce an intrinsic region in which the | electrons and holes would be able to reach the contact |
the nucleus minus the number of inner shell | electrons and is always a positive value. |
ter released two full-length albums, Ancient | Electrons and Besides, Nothing (B-Sides and Rarities, |
cted for relativistic effects of high energy | electrons, and for their magnetic moment. |
at some of the photons convert into pairs of | electrons and positrons causing a runaway reaction whi |
eventually stopped, leaving a trail of free | electrons and ionized molecules. |
J R Atkinson et al. 1960 Scattering of | Electrons and Positrons by Xenon and Mercury, Proceedi |
"low-spin" since filling an orbital matches | electrons and reduces the total electron spin. |
icon CMOS and CCD sensors, some diffusion of | electrons and loss of sharpness in the longer waveleng |
field, i.e. if the difference between solar | electrons and protons gets higher, then earth's magnet |
Oxygen has 6 valence | electrons and prefers to share two electrons in bondin |
purports to show the derivation of photons, | electrons, and U(1) gauge charge, small (relative to t |
Electrons and holes are both fermions with half intege | |
In solid state physics the properties of | electrons and potentials are determined by the spheric |
m, depending upon the number and spin of the | electrons and the orbitals they occupy. |
Nanoscale Structure and Dynamics: Neutrons, | Electrons, and X-rays |
ccur near the electrode which could transfer | electrons, and that the only Van der Waals interaction |
ssume that the whole of space is filled with | electrons and flying electric ions of all kinds. |
ctor walls, the SST-Foil should only measure | electrons and the SST-Open only ions. |
e processes by which mobile charge carriers ( | electrons and electron holes) are created and eliminat |
PsH is constructed from one proton, two | electrons, and one positron. |
ed in the Sun's core when X-rays scatter off | electrons and protons in the presence of strong electr |
so does the surface area hit by the beam of | electrons and therefore the strength of the detected s |
ncharged gas molecules will lose one or more | electrons and become charged ions. |
H. Stanley Allen, | Electrons and Waves: An Introduction to Atomic Physics |
the FIB's two imaging modes, using secondary | electrons and secondary ions, both produced by the pri |
Impurities in the crystals trapped | electrons and holes, ruining the performance of the de |
to the junction, because the populations of | electrons and/or holes are not even in approximate the |
In this Feynman diagram, | electrons annihilate and become a quark-antiquark pair |
other words, knowing where all the previous | electrons appeared on the screen and in what order tel |
Two | electrons are required to fully reduce the loosely bou |
The | electrons are accelerated towards a positively charged |
In the electron gun, the free | electrons are gained by thermo-emission from a hot met |
accelerator of the microtron type, in which | electrons are accelerated to relativistic velocities. |
These | electrons are in resonance with the N-1 nitrogen, dist |
This is the case, for example, when the | electrons are close to a metal-insulator transition. |
In stage I, | electrons are accelerated effectively to energies of t |
As the superconducting | electrons are described by a single coherent wavefunct |
When | electrons are required, the x-ray target is retracted |
The | electrons are drifted by an electric field toward an a |
Collectively, these | electrons are defined as delta radiation when they hav |
Debye sheath is reduced, the more energetic | electrons are able to overcome the potential barrier o |
rome c peroxidase, the compounds that donate | electrons are very specific, because there is a very c |
r the mercury pulls free of the glass, these | electrons are released from the glass into the surroun |
increasing effective nuclear charge since f | electrons are not well shielded, compared to d electro |
Elements of the series in which the | electrons are in 4f orbitals belong to the lanthanide |
The binding energies of the measured | electrons are characteristic of the chemical structure |
of metallic bonding, where valence (bonding) | electrons are delocalized and can flow freely between |
is region a considerable part of the ambient | electrons are accelerated to energies of several tens |
nt meaning since the rules used for counting | electrons are different: every electron belongs to the |
Alternatively, the case where both | electrons are retained by one product is known as hete |
is prohibited, the fast carriers (often the | electrons) are slowed down and the slow carriers (ofte |
and or hydrogen exhibiting a valence pair of | electrons) are responsible for the sensitization of ni |
that work on different principles and which | electrons are highly relativistic. |
ger number of secondary and/or backscattered | electrons are generated on a surface that is not purel |
ave a mass 17, and provided no other nuclear | electrons are gained or lost in the process, an atomic |
as you move across a period, the outer-shell | electrons are pulled more and more strongly towards th |
The | electrons are thought to be transferred along pili (ex |
In condensed matter physics, | electrons are typically described with reference to a |
s as main-group elements because the valence | electrons are in ns2 orbitals. |
However, these | electrons are slowed down through collisions with the |
Electrons are essentially unaffected by the foil. | |
urrent is passed through the MEA protons and | electrons are generated at the anode. |
The optical radiation emitted when | electrons are hitting a metal surface is named "Lilien |
Polarized | electrons are fired at polarized gas targets. |
The delocalized | electrons are free to move throughout the plane. |
at which the constituent atomic nucleus and | electrons are apparent. |
This is permissible since the | electrons are lighter and more mobile than the ions, p |
Non-interacting | electrons are therefore typically described by Bloch w |
ith high electron density or in a void where | electrons are scarce or absent. |
In these ions, two | electrons are delocalized over more than two atoms, re |
ring is similar to Rutherford Scattering but | electrons are used instead of Alpha particles as they |
n autoionize when either two or more valence | electrons are excited or one or more inner-shell elect |
The | electrons are generally trapped in localized states (l |
plasma oscillations) or when the | electrons are prevented from moving by a magnetic fiel |
Inside the Linac, | electrons are focused and accelerated to form a beam o |
Electrons are assumed to have a mobility 3 times large | |
y emitted per unit volume and time when free | electrons are captured from ions to recombinate into n |
This indicates that the pi | electrons are localized and therefore not considered t |
When | electrons are fired singly through a double-slit appar |
Electrons are transported through an external circuit | |
highest range of electron energies in which | electrons are normally present at absolute zero temper |
Electrons are taken from NADPH via TrxR and are transf | |
will become trapped in much the same way as | electrons are observed to be trapped under Anderson lo |
pen suggesting the presence of delocalised π | electrons arising from a conjugation between the benze |
proven experimentally in 2009 that a mass of | electrons artificially confined in a small space toget |
onventional microscopes which use photons or | electrons as the emitting source. |
tensity and angular distributions of emitted | electrons as well as on the total and partial ion yiel |
ses, there was an abrupt cutoff of energetic | electrons as Cassini crossed into the moons' plasma sh |
ep the field emission probes which will emit | electrons as soon as a voltage is applied across it. |
e Sunyaev-Zel'dovich effect, which is due to | electrons associated with gas in galaxy clusters scatt |
We can model the | electrons at the sheath edge with a Boltzmann distribu |
For | electrons at lower energies (below few tens of MeVs), |
ding refers to the local change in energy of | electrons at a semiconductor junction due to space cha |
ory, is needed to understand the behavior of | electrons at such short distance scales, thus the clas |
ton) on an x axis plane to collect and shoot | electrons at a spinning atom to obtain a new atom. |
Davisson and Lester Germer fired slow moving | electrons at a crystalline nickel target. |
00 years ago) was so bright that it stripped | electrons away from the atoms in the gas in its path, |
The more electronegative oxygen atom pulls | electrons away from the carbon forming a greater elect |
Finally k is the wavenumber as the | electrons bands are in wavenumber-space. |
is an excellent electrical insulator, these | electrons become temporarily trapped within the specim |
the laser lost most of its energy in the hot | electrons being generated early in the heating process |
Electrons, being of like charge, repel each other. | |
In an ordinary covalent bond a pair of | electrons bonds two atoms together, one at either end |
leon), nuclear reactions and (especially for | electrons) bremsstrahlung and Cherenkov radiation cont |
sults that indicated particles behaving like | electrons, but with a positive charge, though the resu |
kobeltsyn detected particles that acted like | electrons but curved in the opposite direction in an a |
In AFM, the atoms are probed not by | electrons, but by a sharp vibrating tip. |
re more rapid, because the halogen withdraws | electrons by induction and makes remaining hydrogens m |
pproximation of the diffraction of a beam of | electrons by atomic nuclei is an extension of Mott sca |
The oxidised chlorophyll a replaces the | electrons by photolysis that involves the reduction of |
As only one of the | electrons can be transferred from the QH2 donor to a c |
rypanothione reductase is the sole path that | electrons can take from NADPH to these antioxidant enz |
one of the two ways in which the spin of two | electrons can be combined; the other being a triplet. |
Germer (1896-1971), Davisson discovered that | electrons can undergo diffraction, in accordance with |
Ejected | electrons can escape only from a depth of approximatel |
derivation of the Boltzmann relation for the | electrons can be obtained using the momentum fluid equ |
As is further explained below, backscattered | electrons can also be detected by the signal-gas inter |
Electrons can collide with and scatter from anything t | |
The | electrons can also drop back to ground state after a l |
The pair of | electrons can comprise either a covalent bond, or a lo |
problem by making the gap narrow enough that | electrons can tunnel across the gap, carrying the heat |
The scattering of these | electrons can excite the electronic structure of the s |
Electrons can move (slowly) through an insulator by th | |
band substantially, with the result that the | electrons cannot pass this edge. |
le, when oscillations occur so fast that the | electrons cannot find a new equilibrium (see e.g. |
rmionic emission cooling in that fast moving | electrons carry heat across a gap but cannot return du |
nductive as a result of delocalization of pi | electrons caused by conjugation over all or part of th |
transverse acceleration to the relativistic | electrons, causing them to emit synchrotron radiation. |
d, in order to minimize the diffusion of the | electrons coming from the ionization of the gas. |
al structure to the behavior of the orbiting | electrons, confining them to certain circular (and lat |
In a plasma the free | electrons constantly produce bremsstrahlung in collisi |
versity of Birmingham in England showed that | electrons could jump past each other by quantum tunnel |
versity of Birmingham in England showed that | electrons could jump from the surface of the metal ont |
AC-MIT experiments showed that higher energy | electrons could be scattered through much higher angle |
The | electrons created in this process drift toward a reado |
The covalent | electrons creating this bond move to attack the hydrog |
While most of the high-energy | electrons derived from water are utilized by the cyano |
Some of the | electrons derived from the inorganic donors also need |
Octahedral low-spin: no unpaired | electrons, diamagnetic, substitutionally inert. |
It can be observed how | electrons diffuse away form the surface faster than ho |
It donates | electrons directly to molecular oxygen, thereby produc |
Having 6 π | electrons, dithietes are aromatic. |
In other words, the charge of one mole of | electrons, divided by the number of electrons in a mol |
Electrons do not penetrate as deeply into matter as X- | |
In this model | electrons don't circulate as in Bohr model, but make a |
xin peroxidase (TryP) reduce peroxides using | electrons donated either directly from trypanothione, |
This article clarifies (‽) that | electrons don't actually move in their orbitals. |
This cascade of recombined | electrons, down the Sr+ energy levels, continues freel |
When these | electrons drop back to their former energy levels they |
be, the tritium gives off a steady stream of | electrons due to beta decay. |
At coronal temperatures, | electrons, due to their much smaller mass, reach escap |
The heme iron serves as a source or sink of | electrons during electron transfer or redox chemistry. |
high-latitude boundary of trapped energetic | electrons during a magnetically disturbed period. |
am is aimed towards an acrylic specimen, the | electrons easily penetrate the surface of the acrylic, |
Electrons emerging from the accelerator have energies | |
If the | electrons emit a light wave which is 90° out of phase |
al electronic forces, including the incoming | electrons emitted by the SEM machine, local charge var |
pectroscopy, refers to energy measurement of | electrons emitted from solids, gases or liquids by the |
de (plate) is high enough to collect all the | electrons emitted from the hot cathode. |
e a very accurate spectrum of the numbers of | electrons emitted with energies very close to this tot |
Electrons emitted at any point are accelerated a modes | |
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