Plasmonic photocathode emitters for ultraviolet and visible wavelengths

Abstract

To increase quantum efficiency (QE) of a photocathode.SOLUTION: A photocathode emitter may include a transparent substrate, a photocathode layer, and an array of plasmonic structures disposed between the transparent substrate and the photocathode layer. The plasmonic structure can serve as a spot confinement structure as well as an electrical underlayer for biasing the photocathode. The plasmonic structure can confine incident light at sub-wavelength sizes.SELECTED DRAWING: Figure 8

Description

[Technical field]

[0001] This disclosure relates to photocathode emitters. [Background technology]

[0002] (CROSS-REFERENCE TO RELATED APPLICATIONS) This application claims priority to U.S. Provisional Patent Application No. 62 / 806,822, filed February 17, 2019, the disclosure of which is incorporated by reference.

[0003] Advances in the semiconductor manufacturing industry are placing increasing demands on yield management, particularly on metrology and inspection systems. Not only are critical dimensions continuing to shrink, but the industry is also under pressure to achieve higher yields and higher value production in shorter times. Reducing the total time between detecting a yield problem and correcting it is critical to the return on investment for semiconductor manufacturers.

[0004] In manufacturing semiconductor devices, such as logic and memory devices, semiconductor wafers are typically processed using a number of manufacturing processes to form the various features and multiple levels of the semiconductor devices. For example, a semiconductor manufacturing process known as lithography transfers a pattern from a reticle onto a photoresist array on the semiconductor wafer. Further examples of semiconductor manufacturing processes include, but are not limited to, chemical mechanical polishing (CMP), etching, deposition, and ion implantation. A plurality of semiconductor devices may be fabricated in an array on a single semiconductor wafer, which may then be separated into individual semiconductor devices.

[0005] Electron beams are used in a wide variety of applications in semiconductor manufacturing. For example, an electron beam can be modulated and directed onto electron-sensitive resist on a semiconductor wafer, mask, or other workpiece to generate an electron pattern on the workpiece. Electron beams can also be used to inspect wafers, for example to detect defects, anomalies, or unwanted objects by detecting electrons emitted from or reflected by the wafer.

[0006] These inspection processes are used at various steps during semiconductor manufacturing to help increase the yield and therefore the profitability of the manufacturing process. Inspection has always been an important part of the manufacturing of semiconductor devices, such as integrated circuits (ICs). However, as the dimensions of semiconductor devices decrease, inspection has become ever more important to the successful manufacturing of acceptable semiconductor devices, since even smaller defects can cause device malfunctions. For example, as the dimensions of semiconductor devices decrease, the detection of smaller sized defects becomes necessary, since even relatively small defects can cause unwanted anomalies in those semiconductor devices.

[0007] Photocathodes have been used to generate electron beams. A light beam can be incident on the photocathode system to generate a high-brightness electron beam capable of delivering high electron current density. Planar photocathode structures can be used for applications such as accelerators, electron microscopes, and illumination for lithography or inspection tools, where the photogenerated electron beam may need to be focused to a spot of a few nanometers in size. Due to limitations in electron optics, such a small spot requirement translates into an initial spot size at the photocathode plane that may be limited to subwavelength values ​​even for ultraviolet wavelengths. [Prior art documents] [Patent documents]

[0008] [Patent Document 1] US Patent Application Publication No. 2005 / 0285128 Summary of the Invention [Problem to be solved by the invention]

[0009] Plasmonic structures with photocathodes have been attempted at infrared wavelengths, wavelengths where the most common noble metals used in plasmonics, such as gold and silver, exhibit strong resonances. These structures show that plasmon resonance can enhance the quantum efficiency (QE) of the photocathode at visible or ultraviolet wavelengths (120-700 nm). Although the QE is enhanced, the final QE is still relatively low, even when compared to the QE of metals.

[0010] Improved photocathode emitters are needed. [Means for solving the problem]

[0011] In a first embodiment, a photocathode emitter is provided, which includes a transparent substrate, a photocathode layer, and a plasmonic structure array disposed between the transparent substrate and the photocathode layer.

[0012] The photocathode layer may contain one or more of GaN, an alloy of Al(In)GaN(P), Cs(K)Te(Sb), CsI and CsBr.

[0013] The transparent substrate may contain one or more of UV-fused silica, CaF2, quartz, sapphire, MgF2, and LiF.

[0014] The photocathode emitter can further include a capping layer disposed on an opposite side of the photocathode layer from the array of plasmonic structures, the capping layer can include ruthenium.

[0015] The plasmonic structure may comprise an array of metallic material, which may be aluminum.

[0016] The photocathode emitter may further include a layer between the plasmonic structure array and the photocathode layer, the layer providing lattice matching between the plasmonic structure array and the photocathode layer.

[0017] The photocathode emitter may further include a doped wide bandgap semiconductor layer disposed on the plasmonic structure array opposite the photocathode layer. According to some embodiments, the photocathode emitter may further include a negative electron affinity or a positive electron affinity material. According to some embodiments, the photocathode emitter may further include one or more of Cs, CsBr, CsI, Ba, BaO, and Ba-on flame-retardant oxides. According to some embodiments, the photocathode emitter may further include a dopant, such as at least one of molybdenum and tungsten. The plasmonic structures may define a plurality of plasmonic cavities.

[0018] In a second embodiment, a method is provided by providing a photocathode having a transparent substrate, a photocathode layer, and a plasmonic structure array disposed between the transparent substrate and the photocathode layer, and directing a light beam at the photocathode to generate an electron beam at the photocathode.

[0019] The photocathode can further include a cap layer disposed on an opposite side of the photocathode layer from the array of plasmonic structures.

[0020] The plasmonic structure can include an array of metallic materials.

[0021] The transparent substrate can include a doped wide bandgap semiconductor layer disposed on the array of plasmonic structures opposite the photocathode layer, and in some embodiments, the plasmonic structures define a plurality of plasmonic cavities.

[0022] The photocathode may further include a layer between the plasmonic structure array and the photocathode layer, the layer providing lattice matching between the plasmonic structure array and the photocathode layer.

[0023] For a more complete understanding of the nature and objects of the present disclosure, reference should be had to the accompanying drawings in conjunction with the detailed description which follows. [Brief description of the drawings]

[0024] [Figure 1] 1 is a cross-sectional view of a first embodiment of a photocathode according to the present disclosure. [Diagram 2] FIG. 1 depicts layer thickness optimization calculations for an example plasmonic Al / Cs2Te photocathode. [Diagram 3] FIG. 1 depicts layer thickness optimization calculations for an example plasmonic Al / Cs2Te photocathode. [Figure 4] FIG. 1 depicts layer thickness optimization calculations for an example plasmonic Al / Cs2Te photocathode. [Diagram 5] FIG. 2 is a perspective view of a second embodiment of a photocathode according to the present disclosure. [Figure 6] FIG. 13 is a perspective view of a third embodiment of a photocathode according to the present disclosure. [Figure 7] 1 is a flow chart of a method according to the present disclosure. [Figure 8] FIG. 1 is a block diagram of an embodiment of a system according to the present disclosure. DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

[0025] Although the claimed subject matter is described in terms of certain embodiments, other embodiments are within the scope of this disclosure, including embodiments that do not provide all of the benefits and features described herein. Various structural, logical, process step, and electronic changes can be made without departing from the scope of this disclosure. Accordingly, the scope of this disclosure is to be determined solely by reference to the appended claims.

[0026] To achieve a small laser spot on the photocathode, the disclosed embodiments use plasmonic structures with subwavelength dimensions. Metallic plasmonic structures can act as spot confinement structures and as an electrical underlayer for biasing the photocathode. The plasmonic structures can confine the incident light to subwavelength sizes (e.g., generate electron beams with diameters of 100 nm or less). The plasmonic structures can also be made to have strong resonances at visible and ultraviolet wavelengths, creating high-brightness light sources with high QE for several photocathodes, such as Cs2Te, CsKTe, GaN, CsI, CsBr, and other materials. Metals and other materials, such as aluminum, that have strong plasmon resonances at ultraviolet and visible wavelengths can be used in the plasmonic structures.

[0027] The disclosed embodiments operate at wavelengths where the photocathode exhibits high QE, producing a small spot that allows for a high brightness emitter that is scalable to multiple electron beam arrays.

[0028] In an embodiment, a plasmonic configuration attached to a transmission mode photocathode operating at ultraviolet and visible wavelengths is disclosed. This structure can be operated at wavelengths where the QE of the photocathode is maximized while enhancing optical transmission through the plasmonic aperture to subwavelength spots. Tens of nA can be delivered per beam.

[0029] FIG. 1 is a cross-sectional view of a photocathode 100 according to a first embodiment. The photocathode 100 includes a transparent substrate 101, a photocathode layer 103, and a plasmonic structure array 102 disposed between the transparent substrate 101 and the photocathode layer 103. The photocathode layer 103 can be made of, for example, containing, one or more of GaN, an alloy of Al(In)GaN(P), Cs(K)Te(Sb), CsI, CsBr, and other materials. The transparent substrate 101 can be made of, for example, containing, one or more of UV-fused silica, CaF2, quartz, sapphire, MgF2, LiF, and other materials. The transparent substrate 101 can be transparent at ultraviolet and visible wavelengths. The photocathode layer 103 can exhibit high QE at ultraviolet and visible wavelengths. A high QE photocathode at the wavelength of maximum efficiency can be used to achieve a high brightness emitter. A light source (not shown) can be directed at the photocathode 100, which generates one or more electron beams.

[0030] The plasmonic structure 102 can include an array of metallic materials 105 (shown in FIG. 1 with cross-hatching). The metallic materials 105 can be aluminum, metamaterials, or other materials. Light can be impinged on the metallic materials 105 to generate resonance. The metallic materials 105 can exhibit strong resonances at ultraviolet and visible wavelengths. For example, the strong resonances can correspond to resonance peaks.

[0031] The plasmonic structure 102 and metal material 105 can be scaled to large numbers of electron beams while providing sub-wavelength spots suitable for high throughput inspection systems.

[0032] The photocathode 100 can, but does not have to, include a capping layer 104 disposed on the opposite side of the photocathode layer 103 from the plasmonic structure array 102. The capping layer 104 can be made of, e.g., contain, ruthenium or other low work function metal. For example, the capping layer 104 can contain a ruthenium alloy. The inclusion of a low work function metal in the capping layer 104 can provide long-life operation.

[0033] Although not required, the photocathode 100 may also include a layer (not shown) between the plasmonic structure array 102 and the photocathode layer 103 that provides lattice matching between the plasmonic structure array 102 and the photocathode layer 103. This can improve the growth of the various layers in the photocathode 100. This layer between the plasmonic structure array 102 and the photocathode layer 103 can be thin enough to allow the plasmonic field to penetrate the photocathode layer 103, and can be thick enough to provide high quality growth of the photocathode layer 103. The thickness of this optional layer may be, for example, a few nm. As an example, a tapered AlGaN layer of a few nm can be used to provide lattice matching with the GaN-containing photocathode layer 103.

[0034] The thicknesses of the layers of the photocathode 100 can be optimized for optimal electron emission. For example, by monitoring factors during growth, the thicknesses of the layers of the photocathode 100 can be optimized to absorb incident light and avoid excessive scattering of electrons during transport to the surface. The exact thickness and plasmonic structure dimensions can depend on the photocathode material and the wavelength used for photoemission. For example, dimensions can be optimized by simulation to enhance resonance, which can be wavelength and structure dependent. In addition, plasmonic structure dimensions can be optimized based on the target spot size on the photocathode. An example of thickness optimization for an Al / Cs2Te plasmonic photocathode is shown in Figures 2-4.

[0035] For example, in a bull's-eye aperture geometry for the 266 nm resonance, the glass substrate is placed on the bottom and the Cs2Te layer on top. Light is incident from the substrate side. In this example, the aluminum thickness (h) is 50 nm and the semiconductor thickness (hs) is 15 nm.

[0036] The brightness of the photocathode emitters disclosed herein may depend on the photocathode material and excitation wavelength. The brightness is proportional to the total current and inversely proportional to the emissivity of the photocathode material. For the same incident photon flux, the higher the quantum efficiency of the cathode, the higher the current. Usually, there is a trade-off between QE and emissivity. For some cathodes, e.g., GaN, it is possible to have both high QE and low emissivity. To achieve high brightness, it may be necessary to optimize two parameters: low emissivity or transverse energy (e.g., up to 0.3 eV) and high QE or total current (>1 μA / mW).

[0037] In one example, low emissivity can be achieved by lateral energy spread, resulting in a small spot at the photocathode surface. Focusing a nanometer-sized electron beam spot would require an initial spot size of about 100 nm due to limitations in electron optics.

[0038] However, most photocathodes suitable for inspection systems exhibit low QE in the infrared (<10 -5 As a result, previous efforts have achieved only small pA total currents that are not suitable for high throughput, multiple e-beam inspection systems.

[0039] The photocathode 100 can generate an array of sub-wavelength spot-sized electron beams with tens of nA per electron beam. The photocathode 100 can also maximize light transmission at the sub-wavelength spots to achieve high brightness. The brightness of the photocathode 100 can be higher than that of thermal field emitters. The photocathode 100 can be operated at a value that exhibits high QE. QE is primarily the absorption efficiency of a material at a particular wavelength, minus the scattering and recombination losses of photogenerated electrons within the material. For this reason, thickness optimization is typically performed.

[0040] Additionally, the photocathode 100 can be expanded into a multi-beam system, limited only by the spatial constraints of the overall device.

[0041] QE is generally a function of wavelength and material dependent: it is primarily the absorption efficiency of the material at a particular wavelength minus the losses due to scattering and recombination of photogenerated electrons within the material, so thickness optimization can be performed.

[0042] FIG. 5 is a perspective view of a photocathode according to a second embodiment, and FIG. 6 is a perspective view of a photocathode according to a third embodiment. These are modifications of the photocathode 100 of FIG. 1. The photocathode of FIG. 5 and FIG. 6 is a submicron arrayed low energy diffuse photocathode electron source. The plasmonic structure of FIG. 5 and FIG. 6 can increase the light absorption efficiency to over 80%. Barium combined with a rare earth metal oxide can be used as part of the negative electron affinity (NEA) layer. A non-layered structure of a rare earth metal oxide and a suitable conductor can be used as a doped insulating structure. For example, the metal oxide can be Al2O3 or Sc2O3. The dopant can be molybdenum or tungsten.

[0043] The photocathode 200 of Figure 5 includes a low temperature GaAs thin film 202 on a gold backplane 203. A sub-wavelength gold mesh 201 on the low temperature GaAs thin film 202 includes plasmonic cavities 204. The plasmonic cavities 204 can be round or of other shapes and extend through the sub-wavelength gold mesh 201 and can, but need not, extend into the low temperature GaAs thin film 202. Although gold and GaAs are disclosed, other materials can be used.

[0044] Photocathode 250 of Figure 6 includes a doped wide bandgap semiconductor layer 254 disposed on a plasmonic structure array 253 opposite photocathode layer 252. Plasmonic structure array 253 may include a plurality of plasmonic cavities, such as that shown in Figure 5. Doped wide bandgap semiconductor layer 254 may include dopants such as molybdenum and / or tungsten.

[0045] The photocathode layer 252 can include a NEA or positive electron affinity (PEA) material 252 and can be part of a transparent substrate 257. For example, the photocathode layer 252 can be formed with, e.g., can include, one or more of Cs, CsBr, CsI, Ba, BaO, and Ba-on flame-retardant oxides. For example, the flame-retardant oxide can be Al2O3 or Sc2O3.

[0046] A metal layer 255 can be disposed on the doped wide bandgap semiconductor layer 254. The metal layer 255 can be part of the plasmonic structure array 253 or can be made of the same material as the plasmonic structure array 253.

[0047] Although not required, a thin film electron multiplier (eg, diamond) 251 can be disposed on or near the NEA layer 252. A light source 256 can direct light onto either side of the photocathode 250.

[0048] The photocathode 200 of Figure 5 can be a portion of the photocathode 250 of Figure 6. That is, the GaAs thin film 202 can be an example of the doped wide bandgap semiconductor layer 254, the sub-wavelength gold mesh 201 can be an example of the plasmonic structure array 253, and the gold backplane 203 can be an example of the metal layer 255.

[0049] Photocathode 200 and photocathode 250 achieve improved efficiency due to the additional light absorption and electron delivery through the doped nanolaminate, and extended lifetime due to the high stability of Ba and BaO. Photocathode 200 and photocathode 250 can provide a multi-electron beam system with more than 20 electron beams.

[0050] In the photocathode 250, a plasmonic structure array 253 can be used to increase light trapping efficiency. The NEA or PEA material 252 can be used to lower the surface work function so that electrons can leave the material and enter the vacuum. Nanolaminates (e.g., doping of insulator / wide bandgap semiconductor) can be used to create interstitial states in the doped wide bandgap semiconductor layer 254 to reduce the amount of energy required for photoemission. The nanolaminates can also increase the conductivity of the doped wide bandgap semiconductor layer 254 to improve electron transport. A metal layer 255 can be part of the plasmonic light trap. A light source 256 can be used for illumination and an optional electron multiplier 251 can be used to increase the total electron yield.

[0051] The photocathode 250 can be fabricated by atomic layer deposition (ALD) using Sc2O3 with tungsten or molybdenum nanoparticles as the conductive path for electrons. Barium can be used to form BaO on the surface to lower the surface work function.

[0052] 7 is a flow chart of method 300. In 301, a photocathode is provided, such as one of the photocathode embodiments disclosed herein, which can include a transparent substrate, a photocathode layer, and an array of plasmonic structures disposed between the transparent substrate and the photocathode layer.

[0053] A light beam is directed at the photocathode in 302. An electron beam is generated at the photocathode in 303.

[0054] The photocathode in method 300 can further include a cap layer disposed on an opposite side of the photocathode layer from the array of plasmonic structures.

[0055] The plasmonic structure in method 300 can include an array of metallic materials.

[0056] The transparent substrate in method 300 can have a doped wide bandgap semiconductor layer disposed on the array of plasmonic structures opposite the photocathode layer. The plasmonic structures can define a plurality of plasmonic cavities.

[0057] The photocathode of method 300 can further include a layer between the plasmonic structure array photocathode layers that provides lattice matching between the plasmonic structure array photocathode layers.

[0058] 8 is a block diagram of one embodiment of a system 400. The system 400 includes a wafer inspection tool (including an electron column 401) configured to generate an image of a wafer 404.

[0059] The wafer inspection tool includes a power acquisition subsystem, which includes at least an energy source and a detector. The power acquisition subsystem can be an electron beam power acquisition subsystem. For example, in one embodiment, the energy directed to the wafer 404 is due to electrons, and the energy detected from the wafer 404 is due to electrons. In this manner, the energy source can be an electron beam source. FIG. 8 illustrates one such embodiment, where the power acquisition subsystem includes an electron column 401, which is coupled to a computer subsystem 402. A chuck (not shown) can hold the wafer 404.

[0060] 8, electron column 401 includes an electron beam source 403 configured to generate electrons that are focused by one or more elements 405 onto wafer 404. Electron beam source 403 may include, for example, embodiments of photocathode 100 of FIG. 1, photocathode 200 of FIG. 5, or photocathode 250 of FIG. 6. One or more elements 405 may include, for example, a gun lens, an anode, a beam limiting aperture, a gate valve, a beam current selection aperture, an objective lens, and a scanning subsystem, any of which may include any type of element known and suitable in the art.

[0061] Returning electrons (e.g., secondary electrons) from wafer 404 may be focused onto detector 407 by one or more elements 406. One or more elements 406 may include, for example, a scanning subsystem, which may be the same as the scanning subsystem included in element(s) 405.

[0062] The electron column may incorporate any other suitable elements known in the art.

[0063] 8 is configured such that electrons are directed at the wafer 404 at one oblique angle of incidence and scattered from the wafer 404 at another oblique angle, the electron beam may be directed at and scattered from the wafer 404 at any suitable angle. In addition, the electron beam output acquisition subsystem may be configured to generate images of the wafer 404 using multiple modes (e.g., with different illumination angles, collection angles, etc.). The multiple modes of the electron beam output acquisition subsystem may differ in some imaging parameter of the output acquisition subsystem.

[0064] The computer subsystem 402 may be coupled to a detector 407, which places the computer subsystem 402 in electronic communication with the detector 407 and other components of the wafer inspection tool. By detecting electrons returning from the surface of the wafer 404 with the detector 407, electron beam images of the wafer 404 may be formed by the computer subsystem 402. These electron beam images may include any suitable electron beam images. The computer subsystem 402 includes a processor 408 and an electronic data storage unit 409. The processor 408 may include a microprocessor, a microcontroller, or other device.

[0065] It should be noted that FIG. 8 is provided herein to generally depict an e-beam power acquisition subsystem configuration that may be used in the embodiments described herein. As is commonly done when designing a commercial power acquisition system, an e-beam based power acquisition subsystem having the configuration described herein may be modified to optimize the performance of the power acquisition subsystem. Additionally, the systems described herein may be implemented using existing systems (e.g., by adding the functionality described herein to an existing system). In such systems, the methods described herein may be provided as optional features of the system (e.g., in addition to other features of the system). Alternatively, the systems described herein may be designed as entirely new systems.

[0066] The computer subsystem 402 may be coupled to the components of the system 400 in any suitable manner (e.g., via one or more transmission media, including, for example, wired and / or wireless transmission media) such that the processor 408 may receive its output. The processor 408 may be configured to use the output to perform a number of functions. The wafer inspection tool may receive instructions and other information from the processor 408. Although not required, the processor 408 and / or electronic data storage unit 409 may be in electronic communication with other wafer inspection tools, wafer metrology tools, or wafer review tools (not shown) to receive additional information or send instructions.

[0067] Computer subsystem 402, other system(s), or other subsystem(s) described herein may be part of a variety of systems, including personal computer systems, image computers, mainframe computer systems, workstations, network appliances, Internet appliances, or other devices. The subsystem(s) or system(s) may include any suitable processor known in the art, such as a parallel processor. In addition, the subsystem(s) or system(s) may include high speed processing platforms and software, whether stand-alone or networked tools.

[0068] The processor 408 and electronic data storage unit 409 may be located within or be part of the system 400 or other device. As an example, the processor 408 and electronic data storage unit 409 may be part of a stand-alone control unit or within a centralized quality control unit. Multiple processors 408 or electronic data storage units 09 may be used.

[0069] Processor 408 may be implemented as any combination of hardware, software, and firmware, and its functionality as described herein may be performed in a single unit or distributed among several different components, each of which may in turn be implemented as any combination of hardware, software, and firmware. Program codes or instructions for causing processor 408 to perform and implement various methods and functions may be stored in a readable storage medium, such as a memory in electronic data storage unit 409 or other memory.

[0070] The system 400 of FIG. 8 is merely one example of a system in which the electron source 100 of the embodiments or the method 300 of the embodiments may be used. The system 400 may operate in an ultra-high vacuum (UHV) environment or other environments. The electron source 100 of the embodiments may be part of a defect review system, an inspection system, a metrology system, or any other type of system. That is, the configurations described in accordance with the embodiments of the present disclosure may be tailored in various ways for systems with different capabilities and more or less suitable for different applications.

[0071] The photocathode embodiments disclosed herein can be used in reticle and wafer inspection systems, electron beam inspection systems for wafers or reticles using one or more electron sources, electron beam review systems for wafers or reticles using one or more electron sources, or electron beam metrology systems for wafers or reticles using one or more electron sources. The photocathode embodiments disclosed herein can be used in electron source based systems that use one or more electron sources to generate x-rays, such as those for metrology, review, or inspection of wafers or reticles. For example, the disclosed embodiments can be used in multi-electron source inspection systems or lithography systems.

[0072] Although the present disclosure has been described with reference to one or more specific embodiments, it will be understood that other embodiments of the present disclosure may be made without departing from the scope of the present disclosure, and therefore, the present disclosure is deemed to be limited only by the appended claims and the reasonable interpretation thereof.

Claims

1. A photocathode emitter, A transparent substrate, the transparent substrate comprising: a photocathode layer; and a plasmonic structure array disposed on the photocathode layer; and a doped wide band gap semiconductor layer disposed on the array of plasmonic structures; and a metal layer disposed on the doped wide bandgap semiconductor layer; A photocathode emitter comprising:

2. 2. The photocathode emitter of claim 1, wherein the transparent substrate is made of UV fused silica, CaF ２ , quartz, sapphire, MgF ２ and LiF.

3. 2. The photocathode emitter of claim 1, wherein the photocathode layer comprises a negative electron affinity or a positive electron affinity material.

4. 4. The photocathode emitter of claim 3, wherein the photocathode layer comprises one or more of the following: Cs, CsBr, CsI, Ba, BaO, and Ba-on flame-retardant oxide.

5. 2. The photocathode emitter of claim 1, wherein the doped wide bandgap semiconductor layer contains a dopant, the dopant being at least one of molybdenum and tungsten.

6. 10. The photocathode emitter of claim 1 , wherein the plasmonic structure defines a plurality of plasmonic cavities.

7. The photocathode emitter of claim 1, further comprising: A layer between the plasmonic structure array and the photocathode layer The photocathode emitter has a layer which is responsible for lattice matching between the plasmonic structure array photocathode layers.

8. 8. The photocathode emitter of claim 7, The photocathode layer comprises one or more of GaN, an alloy of Al(In)GaN(P), Cs(K)Te(Sb), CsI and CsBr.

9. 8. The photocathode emitter of claim 7, The transparent substrate is made of ultraviolet fused silica, CaF ２ , quartz, sapphire, MgF ２ and LiF.

10. 8. The photocathode emitter of claim 7, A photocathode emitter, wherein the plasmonic structure comprises an array of metallic material.

11. 11. The photocathode emitter of claim 10, The photocathode emitter, wherein the metallic material is aluminum.

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