Graphene Protected Diamondoid Photocathodes

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Presentation transcript:

Graphene Protected Diamondoid Photocathodes Diamondoids: Molecular-size diamond particles, surface coating via ALD Zhi-Xun Shen Group at Stanford W. L. Yang et al. Monochromatic electron photoemission from diamondoid monolayers. Science 316, 1460 (2007) W. A. Clay et al. The origin of monochromatic photoemission peak in diamondod monolayer. Nano Lett. 9, 56 (2009) H. Ishiwata et al. Diamondoid coating enables disruptive approach for chemical and magnetic imaging with 10 nm spatial resolution. Appl. Phys. Lett. 101, 163101 (2012) P. R. Schreiner et al. Overcoming lability of extremely long alkane carbon-carbon bonds through dispersion forces. Nature 477, 308 (2011) Goals: Engineered work function Generate monochromatic beam using direct photoemission from diamondoid monolayer Air stable diamondoids, operationally stable graphene protective coating Technical challenges: Weak anchoring can lead to dissociation in operation -> graphene coating Improving uniformity of hot-spot dominated emission Effect on emittance needs to be considered Not sure but maybe: ~100 nm vertical roughness over ~100 nm horizontal spacing?

Graphene Protected Diamondoid Photocathodes negative electron affinity (NEA) + strong e-ph coupling + high transmittance of photons and electrons -> give rise to monochromatic photoemission without energy filtering hv e Substrate Diamondoid monolayer Vacuum 1 Photo-excitation Evac Energy 2 Relaxation by e-ph scattering 3 Spontaneous emission NEA level 70% electrons within the NEA peak! Question: 30% is in a very long high energy tail?

Graphene Protected Diamondoid Photocathodes Bare Au 3 eV WF reduction Au + diamondoid monolayer Monolayer diamondoid coating reduces the WF of Au by 3 eV Size / species of diamondoid may change WF shift Effect is comparable to Cs on Au yet air stable Effect is believed to derive from the creation of a surface dipole