Apparatus and method for electron spin polarization detection

Claim 3

A device according to claim 1 further comprising signal enhancing means for enhancing the signal of the scattered electrons from said target, said enhancing means being disposed between said collecting means and said target.

Claim 4

A device according to claim 2 where said enhancing means is at least one electron multiplier plate.

Claim 5

A device according to claim 1 further comprising angle control means for adjusting the size of the solid angle of the electrons diffusely scattered by the target means and which are collected by the collecting means.

Claim 6

A device according to claim 4 where the target means is composed of polycrystalline gold and electrons with scattering angles between 125° and 155° are passed to the collecting means.

Claim 7

A device according to claim 1 where said collecting means is divided into a plurality of sectors for measuring the scattering asymmetry relative to the electron beam.

Claim 8

A device according to claim 1 further comprising means to prevent low energy secondary electrons generated from said target means from reaching said collecting means.

Claim 9

A device according to claim 7 where said means comprises at least one electrified grid disposed between said target means and said collecting means.

Claim 10

A device according to claim 1 where said target means comprises a polycrystalline metal.

Claim 11

A device according to claim 1 where said target means comprises an amorphous metal.

Claim 12

A device according to claim 1 where said target means comprises a polycrystalline semiconductor.

Claim 13

A device according to claim 1 where said target means comprises an amorphous semiconductor.

Claim 14

A device according to claim 1 further comprising a second target means and collecting means disposed perpendicularly to the first target and collecting means and a means for switching the electron beam to impinge on said second target such that all three components of the polarization vector can be determined.

Claim 15

A device according to claim 1 further comprising means for selecting a desired range of kinetic energy of said beam.

Claim 16

A device according to claim 1 further comprising a second target means and collecting means disposed at an angle to the first target and collecting means and a means for switching the electron beam to impinge on said second target such that all three components of the polarization vector can be determined.

Claim 17

A device according to claim 1 where the target means is composed of a polycrystalline or amorphous material.

Claim 18

A device according to claim 1 further comprising concentric means to adjust the angle of collection of electrons scattered from the target.

Claim 23

A method according to claim 19 including the further steps of scattering electrons from a second target and measuring the three components of the polarization vector.

Claim 24

A method according to claim 19 further including the step of changing the longitudinal beam polarization to a transverse beam polarization.

Claim 25

A method according to claim 19 further including the step of rejecting low energy secondary electrons emitted from the target.

Claim 26

A method according to claim 22 further including the step of enhancing the signal produced by the scattered electrons emitted from the target.

Claim 27

A method according to claim 19 further including the step of adjusting the solid angle of collection of the diffusely scattered electrons.

Claim 28

A method according to claim 24 further including the step of selecting scattered electrons having a predetermined range of kinetic energy.

Claim 29

An electron spin polarization detector for magnetic domain structure analysis, achieving a figure of merit of a magnitude of approximately or greater than 10 -4 , comprising: (a) means for providing an elelctron beam to impinge on the target, (b) means for adjusting the electron beam to have an energy of less than 10,000 electron volts, (c) means for maintaining energy of the electrons to within a range of 100 electron volts, (d) target support means for supporting a selected target, (e) target means for incoherently scattering electrons within a large selected solid angle, said target means being supported by said target support means, (f) collector means for collecting the incoherently scattered elecltrons within said large selected solid angle, and (g) detector means for detecting the number and relative position of the scattered electrons to measure spin dependent asymmetry.

Claim 30

An electron spin polarization detector for magnetic domain structure analysis, achieving a figure of merit of a magnitude of approximately or greater than 10 -4 , comprising: (a) means for providing an elelctron beam to impinge on the target, (b) means for adjusting the electron beam to have an energy of less than 10,000 electron volts, (c) means for maintaining energy of the electrons to within a range of 100 electron volts, (d) target support means for supporting a selected target, (e) target means for incoherently scattering electrons within a large selected solid angle, said target means being supported by said target support means, (f) collector means for collecting the incoherently scattered elecltrons within said large selected solid angle, and (g) detector means for detecting the number and relative position of the scattered electrons to measure spin dependent asymmetry.

Claim 31

A detector according to claim 26 where the detector means is divided into sectors.

Claim 32

A detector according to claim 26 further comprising a shield and electrode to permit adjustment of said large selected solid angle over which the scattered electrons are collected.

Claim 33

A detector according to claim 26 further including electron energy selection means disposed between the target support means and the collector means for selecting and passing through to the collector means only scattered electrons of selected energy.

Claim 34

A detector according to claim 29 where the electron energy selection means comprises an electrified grid.

Claim 35

An electron spin polarization detector for analysis of magnetic domains of a sample, comprising: (a) a target composed of a polycrystalline or amorphous material selected from the group consisting of gold, platinum, mercury, lead, bismuth, uranium, or a semiconductor material, (b) target support means for supporting said target, (c) electron beam generation means for generating an electron beam directed to the target where the kinetic energy of the electrons within the electron beam is less than 10,000 electron volts, and within a range of 100 electron volts, (d) means for selecting electrons, emitted in an incoherent pattern from the target, which are within a selected large solid angle, (e) means for selecting electrons which have desired energies, (f) means for collecting and counting the selected electrons within said large solid angle, and (g) means for determining the electron spin polarization of a beam incident on the target.

Claim 36

An electron spin polarization detector for analysis of magnetic domains of a sample, comprising: (a) a target composed of a polycrystalline or amorphous material selected from the group consisting of gold, platinum, mercury, lead, bismuth, uranium, or a semiconductor material, (b) target support means for supporting said target, (c) electron beam generation means for generating an electron beam directed to the target where the kinetic energy of the electrons within the electron beam is less than 10,000 electron volts, and within a range of 100 electron volts, (d) means for selecting electrons, emitted in an incoherent pattern from the target, which are within a selected large solid angle, (e) means for selecting electrons which have desired energies, (f) means for collecting and counting the selected electrons within said large solid angle, and (g) means for determining the electron spin polarization of a beam incident on the target.

Claim 37

A detector according to claim 31 further comprising depositing means for producing the target featuring an electrifiable filament.

Claim 38

Apparatus for analysis of spin polarization, comprising: (a) a target composed of polycrystalline or amorphous material selected from the group consisting of gold, platinum, mercury, lead, bismuth, uranium or a semiconductor material, (b) electron beam generator, (c) electron beam energy control means for controlling beam energy to less than 10,000 electron volts and within a range of 100 electron volts, (d) electron beam focusing means for focusing the electron beam on the target, (e) electron selector means for selecting electrons diffusely scattered from said target upon impingement of the electron beam, said selector means allowing electrons of only sufficient kinetic energy to pass through the selector to the collector means, (f) collector means for collecting electrons passing through the selector means, said collector means being sectored to permit detection of electron spin assymmetry, and (g) means for analyzing and recording the detected electron assymmetry.

Claim 39

Apparatus for analysis of spin polarization, comprising: (a) a target composed of polycrystalline or amorphous material selected from the group consisting of gold, platinum, mercury, lead, bismuth, uranium or a semiconductor material, (b) electron beam generator, (c) electron beam energy control means for controlling beam energy to less than 10,000 electron volts and within a range of 100 electron volts, (d) electron beam focusing means for focusing the electron beam on the target, (e) electron selector means for selecting electrons diffusely scattered from said target upon impingement of the electron beam, said selector means allowing electrons of only sufficient kinetic energy to pass through the selector to the collector means, (f) collector means for collecting electrons passing through the selector means, said collector means being sectored to permit detection of electron spin assymmetry, and (g) means for analyzing and recording the detected electron assymmetry.