1980
DOI: 10.1103/physrevb.22.1972
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Photoemission and optical processes in multialkali photocathodes

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Cited by 24 publications
(15 citation statements)
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“…The electronic structure calculations on the alkali antimonides have remained the central point of attention in the theoretical studies [12][13][14][15][16][17][18][19]. Ghosh [13] used the empirical pseudopotential method for calculating the band structure and the electronic properties of Cs 3 Sb. The theoretical study on the structural stability of the alkali antimonides along with the intermetallic compounds have been done by Christensen [14] using the linear muffin tin orbital (LMTO) method.…”
Section: Introductionmentioning
confidence: 99%
“…The electronic structure calculations on the alkali antimonides have remained the central point of attention in the theoretical studies [12][13][14][15][16][17][18][19]. Ghosh [13] used the empirical pseudopotential method for calculating the band structure and the electronic properties of Cs 3 Sb. The theoretical study on the structural stability of the alkali antimonides along with the intermetallic compounds have been done by Christensen [14] using the linear muffin tin orbital (LMTO) method.…”
Section: Introductionmentioning
confidence: 99%
“…The band structure have been calculated by empirical pseudopotential method and pseudopotential [11]. Christensen [26] have used the linear muffin tin orbitals method in the atomic sphere approximation (LMTO-ASA) to study the structural phase stability of a series of intermetallic compounds including the alkali antimonides.…”
Section: Introductionmentioning
confidence: 99%
“…Since the earlier investigation [1][2][3][4][5][6][7][8], alkali antimonide compounds have attracted much attention and extensive experimental studies on their properties have been carried out [9][10][11][12][13][14][15][16][17][18][19][20][21][22][23][24][25].…”
Section: Introductionmentioning
confidence: 99%
“…The primary cause is an onset of electron-electron (e-e) collisions: e-e scattering events are prevented until the final states of both electrons can reside in the conduction band of K 2 CsSb. 15 This means that for photon energies below the observed peak in QE, electrons excited from the top of the valence band, for example, do not have enough excess energy to scatter with another electron (because their final states would lie within the bandgap). This leaves phonon scattering as the only scattering mechanism and QE continues to rise with increasing incident photon energy until the final states of two collisional electrons can both lie in the conduction band.…”
Section: Photoemission Measurementsmentioning
confidence: 99%