Microdischarge image converter

Claim 2

A proximity focused direct view, electro-optical converter for converting a target scene lying within the visible to far infrared region of the electro-magnetic spectrum into an enhanced visible image, comprising: photon detector means having input and output surfaces responsive to a preselected band of frequencies; means for focusing a photon image of a target scene onto the input surface of said detector, whereby the photons excite said detector to generate and store charge carriers commensurate with the intensity and location of photons falling upon the input surface; means for generating an electric field; an electron to photon converter means, whereby said electric field generating means causes a discharge of said charge carriers from the output surface of said detector, in the form of electrons, which are focused onto and strike said electron to photon converter means for effecting thereon an enhanced image of the target scene.

Claim 3

The apparatus of claim 1, further including a chopper means for periodically interrupting the flow of photons from the target scene at a prescribed frequency in order to allow the photon detector to properly discharge the accumulated charge carriers, whereby the detector may be again exposed to the scene for recharging the dectector means and repeating the operation.

Claim 4

The apparatus of claim 2, wherein said photon detector means includes a layer of material particularly responsive to the specific frequency of the electro-magnetic spectrum desired and a layer of electron emissive material on the output surface of said detector for effecting the transfer of electrons from the detector to the electron to photon converter means.

Claim 5

The apparatus of claim 3, wherein said electron emissive material consists of isolated portions of the emissive material to provide better transfer of said electrons to said electron to photon converter means.

Claim 6

The apparatus of claim 4, wherein the isolated portion of emissive material form individual electron emitter and are isolated by a material which readily changes its electrical state from an insulator to a conductor upon the application of an electric field, whereupon electrons are released from the surface of the electron emitters as the chopper cuts off the flow of photons falling on the input surface of the photon detector and an electric field is impressed across the electron emitters, whereby the released electrons are accelerated toward the electron to photon converter means for providing an enhanced high resolution image thereon.

Claim 7

The apparatus of claim 5, wherein said electron emitters are configured as pin electrodes, whereby the charge thereon is concentrated near the tip of the pin for effecting a higher concentration of electron flow to the portion of said electron to photon converter having the closest proximity to the tip of the electron emissive pin.

Claim 8

The apparatus of claim 6, wherein said electric field generating means comprises a conductive mesh, which, when energized, creates a field across the emitter isolating material to render the material conductive, thereby connecting the emitters to a predetermined biasing level, whereupon the mesh is de-energized allowing the isolating material to revert back to its insulative state, whereby the detector may be again charged to repeat the cycle.

Claim 9

An electrostatic lens in a controllable electric field environment comprising a cathode and an anode spaced in a parallel relationship. said cathode having input and output surfaces whereupon the input surface is sensitive to an applied electron charge constituting a varying charge density pattern along the surface of the material in accordance with the varying intensity of a representatively applied image with the output surface including a multiple array of electronically isolated emitters for storing the charge carriers commensurate with the intensity and location across the input surface of the electron image imposed on the input surface of the cathode; said anode being placed in close proximity to said cathode such that upon the application of an electric field the stored charge carriers are caused to microdischarge and generate a like charge of varying intensity on the anode, thus focusing and enhancing the charge impinging on the input surface of the cathode.

Claim 10

An electrostatic lens in a controllable electric field environment comprising a cathode and an anode spaced in a parallel relationship. said cathode having input and output surfaces whereupon the input surface is sensitive to an applied electron charge constituting a varying charge density pattern along the surface of the material in accordance with the varying intensity of a representatively applied image with the output surface including a multiple array of electronically isolated emitters for storing the charge carriers commensurate with the intensity and location across the input surface of the electron image imposed on the input surface of the cathode; said anode being placed in close proximity to said cathode such that upon the application of an electric field the stored charge carriers are caused to microdischarge and generate a like charge of varying intensity on the anode, thus focusing and enhancing the charge impinging on the input surface of the cathode.

Claim 11

The electrostatic lens of claim 8, wherein the multiple array of electronically isolated emitters comprise extended surface areas upon which charge carriers are continuously stored on the point of the extended surface areas until microdischarged by the application of an electric field sufficient to pull the charge off the tips for effecting a transfer of the charge pattern to the anode.

Claim 12

The electrostatic lens of claim 9, wherein the electric field applied to the cathode is of a magnitude of the order of 10 4 to 10 6 c/cm.

Claim 13

The electrostatic lens of claim 10, wherein the surface of the anode parallel to the cathode contains a like number of extended surface areas, whereby upon discharge of the stored charges from the output surface of the cathode, the charge is transferred to like positioned extended surfaces on the anode to effect an enhanced and more focused image on the anode than was applied to the input surface of the cathode.