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A given fluorophore may emit at single or multiple wavelengths (creatingan emission spectrum
when a sample of excited gas emits particular frequencies of light ATOMIC THEORY I. II(passive) is createdAn emission spectrum
excitation of ultraviolet lights in the compound(passive) caused bythe emission spectrum
excitation of ultraviolet lights in the BeBq2(passive) caused bythe emission spectrum
excitation of ultraviolet lights in the OXD-7(passive) caused bythe emission spectrum
excitation of ultraviolet lights in the Eu(TTA)3phen(passive) caused bythe emission spectrum
a third ring system ( Figures 4(c ) and 4(dinfluencesthe emission spectrum
a change in the potential difference between the first and second electrodes(passive) are caused bythe emission spectrum
Compositioninfluencesthe emission spectrum
the drive current of the element(passive) caused byemission spectrum
of ultraviolet and visible components(passive) is composedThe emission spectrum
heating or electrifying a gaswill createan emission spectrum
Light is radiated by the Suncreatingan emission spectrum
the analysis of their atomic spectrum(passive) were discovered bythe emission spectrum
when electrons of a hot gas fall from higher energy states to lower energy states , and emit a photon(passive) is createdAn emission spectrum
the random spread of velocities in the gas(passive) caused bythe emission spectrum
Electrons Jumping in Atoms like the sun or stars like interstellar gas or a star 's atmosphere(passive) Caused bySpectrum - Absorbtion Emission
any of the excitation light in the range of wavelengths 430nm~500 nm is irradiatedresultingemission spectrum
atoms emitting photons of light(passive) are caused byEmission spectrum
the type of discharge gas to be filled(passive) can be set byThe emission spectrum
the rotational transition of the atmospheric constituents(passive) caused byan emission spectrum
mode distribution characteristics during high rate modulation and emission wavelength fluctuation due to temperature(passive) caused byemission spectrum fluctuation
the microwave(passive) caused byThe emission spectrum
rarefied gas emitting the(passive) is caused byan emission spectrum
when a gas is heated and very specific wavelengths of light are produced(passive) is createdAn emission spectrum
electron - hole recombination(passive) caused byemission spectrum
the electrodes of HID lampsinfluencethe emission spectrum
photoexcitation of the organic film O.sub.4(passive) caused bythe emission spectrum
electrons dropping to lower atomic energy states ... electromagnetic energy in the form of photons of light is given off in each transition downwards(passive) is caused byAn emission spectrum
photoexcitation of the organic film O.sub.3(passive) caused bythe emission spectrum
the etalon ( FSR ~5 nm , bandwidth ~0.37 nm(passive) set byemission spectrum of the VECSEL
of three peaks at 567 nm , 603 nm and 650 nm(passive) is composedEmission spectrum
the atoms and ions within the plasma(passive) created byan emission spectrum
phase truncation(passive) caused bySpectrum emission
photoexcitation of the organic film O4(passive) caused bythe emission spectrum
photoexcitation of the organic film O3(passive) caused bythe emission spectrum
TNH plasma(passive) caused bythe emission spectrum
the process by whichcreatesan emission spectrum
conditions imposed on the excited state of the molecule , a state in which the equilibrium electronic configuration can be much different from that in the ground state(passive) is influenced byThe emission spectrum
flourescent light spectrum ledfluorescentsunlightcomparisonchartsledlight emission spectrum
of the main emission linecomposedof the main emission line
of a mixture of primary colors having imbalanced emission energy contentscomposedof a mixture of primary colors having imbalanced emission energy contents
Moreover , the excitation wavelength at the time of measuring(passive) was setMoreover , the excitation wavelength at the time of measuring
from the decay of excited States of the material that transform with increasing frequency , eresultingfrom the decay of excited States of the material that transform with increasing frequency , e
substantially of narrow red , green and blue emission peaks ... and that the emission peaks in the spectrum of the nanophosphors in the left hand view of FIG . 2is composedsubstantially of narrow red , green and blue emission peaks ... and that the emission peaks in the spectrum of the nanophosphors in the left hand view of FIG . 2
Initial to true for the d state and false for the a statesetInitial to true for the d state and false for the a state
of a single line with photon energies from 1.26 to 1.55 eV ( 0.98 .mu.m tocomposedof a single line with photon energies from 1.26 to 1.55 eV ( 0.98 .mu.m to
from the energy transition between the levels 7 F1 A2 and 5 D0resultingfrom the energy transition between the levels 7 F1 A2 and 5 D0
from the first emitting layer at the maximum luminescent wavelength and the luminescent intensity ( I2 ) of the emission spectrum originating from the second emitting layer at the maximum luminescent wavelengthoriginatingfrom the first emitting layer at the maximum luminescent wavelength and the luminescent intensity ( I2 ) of the emission spectrum originating from the second emitting layer at the maximum luminescent wavelength
from the transition between the levels 7 F1 A2 and 5 D0 depended on the angular frequency ωex of the excited lightresultingfrom the transition between the levels 7 F1 A2 and 5 D0 depended on the angular frequency ωex of the excited light
from the excitation at various wavelengthsresultingfrom the excitation at various wavelengths
from excitation at 274 nmresultingfrom excitation at 274 nm
from the excitation of the final extractresultingfrom the excitation of the final extract
from X - ray excitationresultingfrom X - ray excitation
from excitation light with light of wavelengthresultingfrom excitation light with light of wavelength
from 458 nm excitation and the red traceresultingfrom 458 nm excitation and the red trace
from the impact excitation of H2 by a 30 eV electronresultingfrom the impact excitation of H2 by a 30 eV electron
a negative Stokes shift ... so its wavelength is shorter than that of excitation radiationcausesa negative Stokes shift ... so its wavelength is shorter than that of excitation radiation
independent of the excitation mode from 1PE to MPE like the quantum efficiencyresultsindependent of the excitation mode from 1PE to MPE like the quantum efficiency
upon excitation of the curable material system or of the article containing the cured material systemresultsupon excitation of the curable material system or of the article containing the cured material system
at an excitation peak wavelength ... and the monitoring wavelength at the time of measuring the excitation spectrum was set at the emission peak wavelengthwas setat an excitation peak wavelength ... and the monitoring wavelength at the time of measuring the excitation spectrum was set at the emission peak wavelength
from electron impact on H[SUB]2[/SUBresultingfrom electron impact on H[SUB]2[/SUB
by electronic transitions from high electronic energy levelsresultby electronic transitions from high electronic energy levels
from the spectral gain function and longitudinal mode positions showncould resultfrom the spectral gain function and longitudinal mode positions shown
from illumination of a substance ( usually a molecular gas ) by radiation of a definite frequency or definite frequenciesresultingfrom illumination of a substance ( usually a molecular gas ) by radiation of a definite frequency or definite frequencies
apparentlyoriginatesapparently
from the extracted emission profileresultingfrom the extracted emission profile
from an effectively narrow bandwidth transducer ( FIGresultingfrom an effectively narrow bandwidth transducer ( FIG
from Tb3originatingfrom Tb3
to the generation of characteristic emission spectral linesleadsto the generation of characteristic emission spectral lines
in white lightresultsin white light
in a desired apparent color ... or to use multimode microcavities to obtain emission wavelengths which match a predetermined filter setto resultin a desired apparent color ... or to use multimode microcavities to obtain emission wavelengths which match a predetermined filter set
at 254 nmwas setat 254 nm
of the photoluminescence of both A1Q and naphtho[2,3-a]pyrenecomposedof the photoluminescence of both A1Q and naphtho[2,3-a]pyrene
from the blendresultingfrom the blend
to a high CRImight contributeto a high CRI
from excited electrons typically returning to their ground stateis createdfrom excited electrons typically returning to their ground state
to an understanding of the existence of discrete electron energy levels in atomsleadsto an understanding of the existence of discrete electron energy levels in atoms
of main emission lines of 3 nm or more and less than 10 nmcomposedof main emission lines of 3 nm or more and less than 10 nm
when an electron in an atom undergoes a transition from excited state to the ground stateresultswhen an electron in an atom undergoes a transition from excited state to the ground state