Pub Date : 1988-07-01Epub Date: 2002-10-09DOI: 10.1016/0378-4363(88)90195-7
Yujiro Koh, Toku Sasaki
To examine experimentally, whether there are differences between the two-beam Dirac self-interferences of massless and massive particles, modifications of the electron biprism and the neutron double-slit interferometer are proposed as follows: (a) extension of the biprism techniques from electron to photon or heavier ions, and (b) macroscopic elongation in the two-beam interferometers, of the total separated path lengths (TSPL) which are different from the conventional path difference.
The idea, that the interference fringes for heavy masses should become more obscure as the TSPL are lengthened, seems to be conceivable for a natural model, which assumes a kind of spontaneous in-flight transition before the so-called observation starts since the arrival at the counter.
The relationships between the in-flight transition and Prigogine's microscopic irreversible scattering are discussed.
{"title":"Are two-beam Dirac interferences mass-independent?","authors":"Yujiro Koh, Toku Sasaki","doi":"10.1016/0378-4363(88)90195-7","DOIUrl":"10.1016/0378-4363(88)90195-7","url":null,"abstract":"<div><p>To examine experimentally, whether there are differences between the two-beam Dirac self-interferences of massless and massive particles, modifications of the electron biprism and the neutron double-slit interferometer are proposed as follows: (a) extension of the biprism techniques from electron to photon or heavier ions, and (b) macroscopic elongation in the two-beam interferometers, of the total separated path lengths (TSPL) which are different from the conventional path difference.</p><p>The idea, that the interference fringes for heavy masses should become more obscure as the TSPL are lengthened, seems to be conceivable for a natural model, which assumes a kind of spontaneous in-flight transition before the so-called observation starts since the arrival at the counter.</p><p>The relationships between the in-flight transition and Prigogine's microscopic irreversible scattering are discussed.</p></div>","PeriodicalId":101023,"journal":{"name":"Physica B+C","volume":"151 1","pages":"Pages 362-365"},"PeriodicalIF":0.0,"publicationDate":"1988-07-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0378-4363(88)90195-7","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"75841487","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 1988-07-01Epub Date: 2002-10-09DOI: 10.1016/0378-4363(88)90168-4
Akira Tonomura
The Aharonov-Bohm effect (AB effect) involves fundamental problems in quantum mechanics such as the reality of vector potentials, the locality of physical effects, and the single-valuedness of the wave function in multiply connected spaces. Therefore various kinds of discussions have continuously been made for these 30 years. In this controversy, some people even negated the existence of the AB effect, attributing the experimental results previously performed to the Lorentz force effect due to the overlap between the electron and the magnetic field. In order to settle this situation, new experiments were carried out and the controversy entered a new phase.
{"title":"New results on the Aharonov-Bohm effect with electron interferometry","authors":"Akira Tonomura","doi":"10.1016/0378-4363(88)90168-4","DOIUrl":"10.1016/0378-4363(88)90168-4","url":null,"abstract":"<div><p>The Aharonov-Bohm effect (AB effect) involves fundamental problems in quantum mechanics such as the reality of vector potentials, the locality of physical effects, and the single-valuedness of the wave function in multiply connected spaces. Therefore various kinds of discussions have continuously been made for these 30 years. In this controversy, some people even negated the existence of the AB effect, attributing the experimental results previously performed to the Lorentz force effect due to the overlap between the electron and the magnetic field. In order to settle this situation, new experiments were carried out and the controversy entered a new phase.</p></div>","PeriodicalId":101023,"journal":{"name":"Physica B+C","volume":"151 1","pages":"Pages 206-213"},"PeriodicalIF":0.0,"publicationDate":"1988-07-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0378-4363(88)90168-4","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"80779444","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 1988-07-01Epub Date: 2002-10-09DOI: 10.1016/0378-4363(88)90180-5
M.P. Silverman
The wave-like attributes of matter have been examined in numerous interference experiments exhibiting the first-order coherence of the particle field. Intensity fluctuation and correlation experiments, such as pioneered in light optics by Hanbury Brown and Twiss, manifest second-order coherence, a measure of particle clustering behaviour. Experiments of this nature have not, as yet, been performed on massive particle beams. The cross-correlation of output beams in a Mach-Zehnder fermion interferometer is sensitive to the coherence properties of multiparticle input states and to the quantum mechanical interaction of such states with potential fields such as electromagnetic potentials or gravity. Examples of both one- and two-port input beams are considered.
{"title":"Quantum interference effects on fermion clustering in a fermion interferometer","authors":"M.P. Silverman","doi":"10.1016/0378-4363(88)90180-5","DOIUrl":"10.1016/0378-4363(88)90180-5","url":null,"abstract":"<div><p>The wave-like attributes of matter have been examined in numerous interference experiments exhibiting the first-order coherence of the particle field. Intensity fluctuation and correlation experiments, such as pioneered in light optics by Hanbury Brown and Twiss, manifest second-order coherence, a measure of particle clustering behaviour. Experiments of this nature have not, as yet, been performed on massive particle beams. The cross-correlation of output beams in a Mach-Zehnder fermion interferometer is sensitive to the coherence properties of multiparticle input states and to the quantum mechanical interaction of such states with potential fields such as electromagnetic potentials or gravity. Examples of both one- and two-port input beams are considered.</p></div>","PeriodicalId":101023,"journal":{"name":"Physica B+C","volume":"151 1","pages":"Pages 291-297"},"PeriodicalIF":0.0,"publicationDate":"1988-07-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0378-4363(88)90180-5","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"82672089","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 1988-07-01Epub Date: 2002-10-09DOI: 10.1016/0378-4363(88)90177-5
G. Dorda
The importance of quantum phenomena in semiconductor components, in particular in Si MOSFETs and GaAlAs/ GaAs heterostructures, is outlined. A short theoretical description of quantization effects in surface potential wells and at high magnetic fields is given. Multiple quantum well structures and modulation-doped heterostructures, as well as their possible applications are described. The discovery of the quantum Hall effect (QHE) is shown to be a result of the development of high-quality components. The features and the importance of the QHE for basic physics are outlined. Recent experimental data are discussed showing that the theoretical description of QHE is still unsatisfactory. A possible analogy of QHE to some features of superconductivity based on the idea of a changed effective mass is considered.
{"title":"Quantum effects in semiconductor components","authors":"G. Dorda","doi":"10.1016/0378-4363(88)90177-5","DOIUrl":"10.1016/0378-4363(88)90177-5","url":null,"abstract":"<div><p>The importance of quantum phenomena in semiconductor components, in particular in Si MOSFETs and GaAlAs/ GaAs heterostructures, is outlined. A short theoretical description of quantization effects in surface potential wells and at high magnetic fields is given. Multiple quantum well structures and modulation-doped heterostructures, as well as their possible applications are described. The discovery of the quantum Hall effect (QHE) is shown to be a result of the development of high-quality components. The features and the importance of the QHE for basic physics are outlined. Recent experimental data are discussed showing that the theoretical description of QHE is still unsatisfactory. A possible analogy of QHE to some features of superconductivity based on the idea of a changed effective mass is considered.</p></div>","PeriodicalId":101023,"journal":{"name":"Physica B+C","volume":"151 1","pages":"Pages 273-278"},"PeriodicalIF":0.0,"publicationDate":"1988-07-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0378-4363(88)90177-5","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"74461758","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 1988-07-01Epub Date: 2002-10-09DOI: 10.1016/0378-4363(88)90148-9
F. Mezei
In some polarized neutron beam experiments, such as Neutron Spin Echo spectroscopy, it is essential to follow exactly the minute changes of the neutron kinetic energy due to interaction with the magnetic fields, e.g. in a spin flip process. It is emphasized that in the Amperian current loop model of microscopic magnetism, shown to be valid by the experiments, the Zeeman energy term can be treated as a bona fide potential energy. This allows us to describe both the spin and the spatial motion of the neutron by using simple notions of wave propagation across potential steps. In this picture Larmor precessions are represented as interference between two Stern-Gerlach states ↑ and ↓. The approach proves to be sufficient for the interpretation of all known polarized neutron beam phenomena, including crystal interferometry. It also leads to the surprising prediction that, as a pure quantum effect, under special circumstances the Larmor precession frequency can be different from its classical value.
{"title":"Zeeman energy, interference and Neutron Spin Echo: A minimal theory","authors":"F. Mezei","doi":"10.1016/0378-4363(88)90148-9","DOIUrl":"https://doi.org/10.1016/0378-4363(88)90148-9","url":null,"abstract":"<div><p>In some polarized neutron beam experiments, such as Neutron Spin Echo spectroscopy, it is essential to follow exactly the minute changes of the neutron kinetic energy due to interaction with the magnetic fields, e.g. in a spin flip process. It is emphasized that in the Amperian current loop model of microscopic magnetism, shown to be valid by the experiments, the Zeeman energy term can be treated as a bona fide potential energy. This allows us to describe both the spin and the spatial motion of the neutron by using simple notions of wave propagation across potential steps. In this picture Larmor precessions are represented as interference between two Stern-Gerlach states ↑ and ↓. The approach proves to be sufficient for the interpretation of all known polarized neutron beam phenomena, including crystal interferometry. It also leads to the surprising prediction that, as a pure quantum effect, under special circumstances the Larmor precession frequency can be different from its classical value.</p></div>","PeriodicalId":101023,"journal":{"name":"Physica B+C","volume":"151 1","pages":"Pages 74-81"},"PeriodicalIF":0.0,"publicationDate":"1988-07-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0378-4363(88)90148-9","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"91756559","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 1988-07-01Epub Date: 2002-10-09DOI: 10.1016/0378-4363(88)90175-1
Peter J. Martin , Phillip L. Gould , Bruce G. Oldaker, Andrew H. Miklich, David E. Pritchard
This paper presents experiments concerning momentum transfer to atoms by a standing light wave in the absence of spontaneous decay. This momentum transfer, which occurs in discrete units of 2 ħ k along the k-vector of the standing light wave, can be viewed as absorption/stimulated emission of photon pairs from the counterpropagating traveling waves which make up the standing light wave. In a dual sense, this phenomenon can also be viewed as diffraction of an atomic de Broglie wave from the periodic intensity grating of the standing light wave. In addition, we address how the inherent Heisenberg uncertainty between the focussed waist of the standing light wave and the angular spread of the k-vectors of photons traveling through this waist affects momentum transfer to the atoms by the light. For large widths of the standing light wave, the reduction of the uncertainty in the direction of the photons results in resonances for the momentum transfer only for discrete values of atomic momentum along the k-vector of the standing light wave which satisfy the Bragg condition. We present experimental data which display the Pendellösung effect for Bragg scattering of atomic de Broglie waves from a standing light wave. Finally, we discuss the possibility of exploiting these phenomena to build an atomic interferometer, one that interferes atomic de Broglie waves.
{"title":"Diffraction of atoms from a standing light wave","authors":"Peter J. Martin , Phillip L. Gould , Bruce G. Oldaker, Andrew H. Miklich, David E. Pritchard","doi":"10.1016/0378-4363(88)90175-1","DOIUrl":"10.1016/0378-4363(88)90175-1","url":null,"abstract":"<div><p>This paper presents experiments concerning momentum transfer to atoms by a standing light wave in the absence of spontaneous decay. This momentum transfer, which occurs in discrete units of 2 ħ <em>k</em> along the <strong><em>k</em></strong>-vector of the standing light wave, can be viewed as absorption/stimulated emission of photon pairs from the counterpropagating traveling waves which make up the standing light wave. In a dual sense, this phenomenon can also be viewed as diffraction of an atomic de Broglie wave from the periodic intensity grating of the standing light wave. In addition, we address how the inherent Heisenberg uncertainty between the focussed waist of the standing light wave and the angular spread of the <strong><em>k</em></strong>-vectors of photons traveling through this waist affects momentum transfer to the atoms by the light. For large widths of the standing light wave, the reduction of the uncertainty in the direction of the photons results in resonances for the momentum transfer only for discrete values of atomic momentum along the <strong><em>k</em></strong>-vector of the standing light wave which satisfy the Bragg condition. We present experimental data which display the Pendellösung effect for Bragg scattering of atomic de Broglie waves from a standing light wave. Finally, we discuss the possibility of exploiting these phenomena to build an atomic interferometer, one that interferes atomic de Broglie waves.</p></div>","PeriodicalId":101023,"journal":{"name":"Physica B+C","volume":"151 1","pages":"Pages 255-261"},"PeriodicalIF":0.0,"publicationDate":"1988-07-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0378-4363(88)90175-1","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"74514380","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 1988-07-01Epub Date: 2002-10-09DOI: 10.1016/0378-4363(88)90194-5
C.W. Rietdijk
We consider a variant of Young's double-slit experiment with polarized photons for which quantum theory predicts that different amounts of angular momentum will be absorbed at a certain location M according as we set up a revolving plate or a Nicol prism at M. This difference, which implies a retroactive effect because angular momentum is a conserved quantity, can in principle be established experimentally. The relevant experiment differs fundamentally from Wheeler's delayed-choice experiments.
Another experiment is also discussed in which retroactivity cannot be expected to manifest, though it is seemingly similar to the first one.
Finally, we consider an analogous experiment with spin particles, in which it can also be expected from quantum mechanics that a retroactive effect will appear. Here, too, experimental verification is in principle possible.
{"title":"A possible experimental verification of retroactivity","authors":"C.W. Rietdijk","doi":"10.1016/0378-4363(88)90194-5","DOIUrl":"10.1016/0378-4363(88)90194-5","url":null,"abstract":"<div><p>We consider a variant of Young's double-slit experiment with polarized photons for which quantum theory predicts that different amounts of angular momentum will be absorbed at a certain location M according as we set up a revolving plate or a Nicol prism at M. This difference, which implies a retroactive effect because angular momentum is a conserved quantity, can in principle be established experimentally. The relevant experiment differs fundamentally from Wheeler's delayed-choice experiments.</p><p>Another experiment is also discussed in which retroactivity cannot be expected to manifest, though it is seemingly similar to the first one.</p><p>Finally, we consider an analogous experiment with spin particles, in which it can also be expected from quantum mechanics that a retroactive effect will appear. Here, too, experimental verification is in principle possible.</p></div>","PeriodicalId":101023,"journal":{"name":"Physica B+C","volume":"151 1","pages":"Pages 358-361"},"PeriodicalIF":0.0,"publicationDate":"1988-07-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0378-4363(88)90194-5","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"78001338","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 1988-07-01Epub Date: 2002-10-09DOI: 10.1016/0378-4363(88)90144-1
A.I. Ioffe
Aberration distortions of wavefronts in a very cold neutron interferometer using diffraction gratings are analyzed. Aberrations that considerably reduce the efficiency of a two-grating interferometer are shown to be fully compensable by adding a third diffraction grating, which also permits the interferometer to operate with a non-collimated and non-monochromatized illuminating beam thereby raising its efficiency. A fourth diffraction grating additionally permits compensation of effects of the terrestrial rotation that affect performance of a large interferometer in which the spatial separation of beams can be of the order of a few meters.
It is demonstrated to be practically possible to implement an interferometer for neutrons having a wavelength λ = 20 Å and to use it in experiments aimed at finding the electric charge of the neutron at the level of 10−23 to 10−22 of the electronic charge.
{"title":"Diffraction-grating neutron interferometers","authors":"A.I. Ioffe","doi":"10.1016/0378-4363(88)90144-1","DOIUrl":"https://doi.org/10.1016/0378-4363(88)90144-1","url":null,"abstract":"<div><p>Aberration distortions of wavefronts in a very cold neutron interferometer using diffraction gratings are analyzed. Aberrations that considerably reduce the efficiency of a two-grating interferometer are shown to be fully compensable by adding a third diffraction grating, which also permits the interferometer to operate with a non-collimated and non-monochromatized illuminating beam thereby raising its efficiency. A fourth diffraction grating additionally permits compensation of effects of the terrestrial rotation that affect performance of a large interferometer in which the spatial separation of beams can be of the order of a few meters.</p><p>It is demonstrated to be practically possible to implement an interferometer for neutrons having a wavelength <em>λ</em> = 20 Å and to use it in experiments aimed at finding the electric charge of the neutron at the level of 10<sup>−23</sup> to 10<sup>−22</sup> of the electronic charge.</p></div>","PeriodicalId":101023,"journal":{"name":"Physica B+C","volume":"151 1","pages":"Pages 50-56"},"PeriodicalIF":0.0,"publicationDate":"1988-07-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0378-4363(88)90144-1","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"91721025","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}