K 2 CsSb Cathode Development John Smedley Triveni Rao Andrew Burrill BNL ERL needs – 50 mA, 7 mm dia., 1.3 mA/mm 2.

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Presentation transcript:

K 2 CsSb Cathode Development John Smedley Triveni Rao Andrew Burrill BNL ERL needs – 50 mA, 7 mm dia., 1.3 mA/mm 2

K 2 CsSb (Alkali Antimonides) D. H. Dowell et al., Appl. Phys. Lett., 63, 2035 (1993) C. Ghosh and B.P. Varma, “J. Appl. Phys., 49, 4549 (1978) A.R.H.F. Ettema and R.A. de Groot, Phys. Rev. B 66, (2002) Work function 1.9eV, E g = 1.2 eV Good QE (4% 532 nm, 355nm) Deposited in Torr vacuum Typically sequential (Sb->K->Cs); Cs deposition used to optimize QE Oxidation to create Cs-O dipole Co-deposition increases performance in tubes Cathode stable in deposition system (after initial cooldown)

Deposition System Sequential deposition with retractable sources (prevents cross-contamination) Cathode mounted on rotatable linear-motion arm Typical vacuum 0.02 nTorr (0.1 nTorr during Sb deposition) SbKCs

Deposition System Laser access from bottom during deposition from front and back for measurement Anode for HV bias (2.5 cm gap, up to 5 kV)

Substrate Copper Substrate Polished Solid Copper ~30 nm Copper Sputtered on Glass Recipe Following D. Dowell (NIM A ) Cool to room temperature as quickly as possible (~15 min) Stainless Steel Shield Stainless Section Substrate Temperature 100 Å Sb150 C 200 Å K140 C Cs to optimize QE 135 C

10 min to cool to 100C Lose 15% of QE

Spectral Response

SS Cath Window Cu Cath SS Shield Cu transmission ~20% Position Scan (532 nm)

nm mA Copper vs Stainless

Temperature Dependence

QE Decay 500 V bias 3 mm diameter spot Current ~ 60µA 0.07 nTorr

Linearity and Space Charge 80 µm FWHM spot on cathode

QE Decay, Small Spot 1.3 mA/mm 2 current density 1.5x10 5 C/mm 2 80 µm FWHM spot on cathode

Conclusions Cathodes have better QE on Stainless than on Cu QE decreases 15% during cathode cool-off QE at 355 nm is 19%, better than the 10% required ERL current density has been met (1.3 mA/mm 2 ) QE does not change in storage (even illuminated) –Ion bombardment seems to limit lifetime under bias QE at -77C same as at 20C Charge density of 1.5x10 5 C/mm 2 extracted from a small (80 µm fwhm) spot; 15 C extracted from a 3 mm fwhm spot; both with small but measurable QE loss Thanks!

Deposition Notes Initial vacuum <0.1 nTorr –Primary contaminants H 2 and Ar Source to substrate distance of ~45 mm Antimony and Potassium deposition rates set by crystal monitor –Crystal monitor to source spacing ~70mm QE measured 532 nm) during Cs deposition Substrate takes 15 min to reach room temperature QE drops rapidly during this period –Initial QE decay occurs prior to QE map, so we may miss peak QE

Alkali Sources Initial attempts with Saes Getters Chromate sources –Could not obtain evaporation below 10A (should be <6.5A) Used Alvasources –Pure Alkali sources, with In seal –Two stage heating cycle –Two geometries – line and V –Ar fill gas produces gas load on initial heating

Reflection QE (543 nm) vs Position SS Guard Transparent Substrate Cu Cathode

Transmission QE (543 nm) vs Position

Energy MediumVacuum Φ Three Step Model - Semiconductors Filled States Empty States h 1) Excitation of e - Reflection, Transmission, Interference Energy distribution of excited e - 2) Transit to the Surface e - -lattice scattering mfp ~100 angstroms many events possible e - -e - scattering (if hν>2E g ) Spicer’s Magic Window Random Walk Monte Carlo Response Time (sub-ps) 3) Escape surface Overcome Electron Affinity Laser No States EgEg EaEa

A.R.H.F. Ettema and R.A. de Groot, Phys. Rev. B 66, (2002)

QE vs Field