Non-Hermitian quantum mechanics (original) (raw)
PT symmetry was initially studied as a specific system in non-Hermitian quantum mechanics, where Hamiltonians are not Hermitian. In 1998, physicist Carl Bender and former graduate student Stefan Boettcher published in Physical Review Letters a paper in quantum mechanics, "Real Spectra in non-Hermitian Hamiltonians Having PT Symmetry." In this paper, the authors found non-Hermitian Hamiltonians endowed with an unbroken PT symmetry (invariance with respect to the simultaneous action of the parity-inversion and time reversal symmetry operators) also may possess a real spectrum. Under a correctly-defined inner product, a PT-symmetric Hamiltonian's eigenfunctions have positive norms and exhibit unitary time evolution, requirements for quantum theories. Bender won the 2017 Dannie Heineman Prize
Property | Value |
---|---|
dbo:abstract | PT symmetry was initially studied as a specific system in non-Hermitian quantum mechanics, where Hamiltonians are not Hermitian. In 1998, physicist Carl Bender and former graduate student Stefan Boettcher published in Physical Review Letters a paper in quantum mechanics, "Real Spectra in non-Hermitian Hamiltonians Having PT Symmetry." In this paper, the authors found non-Hermitian Hamiltonians endowed with an unbroken PT symmetry (invariance with respect to the simultaneous action of the parity-inversion and time reversal symmetry operators) also may possess a real spectrum. Under a correctly-defined inner product, a PT-symmetric Hamiltonian's eigenfunctions have positive norms and exhibit unitary time evolution, requirements for quantum theories. Bender won the 2017 Dannie Heineman Prize for Mathematical Physics for his work. A closely related concept is that of operators, which were considered by physicists Dirac, Pauli, and Lee and Wick. operators were discovered (or rediscovered) almost simultaneously by mathematicians Krein et al. as G-Hamiltonian in the study of linear dynamical systems. The equivalence between pseudo-Hermiticity and G-Hamiltonian is easy to establish. In 2002, showed that every non-Hermitian Hamiltonian with a real spectrum is pseudo-Hermitian. He found that PT-symmetric non-Hermitian Hamiltonians that are diagonalizable belong to the class of pseudo-Hermitian Hamiltonians. However, this result is not useful because essentially all interesting physics happens at the exception points where the systems are not diagonalizable. It was proven recently that in finite dimensions PT-symmetry entails pseudo-Hermiticity regardless of diagonalizability, which indicates that the mechanism of PT-symmetry breaking at exception points, where the Hamiltionian is usually not diagonalizable, is the Krein collision between two eigenmodes with opposite signs of actions. In 2005, PT symmetry was introduced to the field of optics by the research group of Gonzalo Muga by noting that PT symmetry corresponds to the presence of balanced gain and loss. In 2007, the physicist Demetrios Christodoulides and his collaborators further studied the implications of PT symmetry in optics. The coming years saw the first experimental demonstrations of PT symmetry in passive and active systems. PT symmetry has also been applied to classical mechanics, metamaterials, electric circuits, and nuclear magnetic resonance. In 2017, a non-Hermitian PT-symmetric Hamiltonian was proposed by Dorje Brody, and Markus Müller that "formally satisfies the conditions of the Hilbert–Pólya conjecture." (en) A mecânica quântica não-hermitiana é uma mecânica quântica que pode ser construída sobre um hamiltoniano complexo que não é hermitiano, mas que satisfaz a condição física da simetria de reflexão espaço-tempo. A mecânica quântica não-hermitiana aparece no estudo de sistemas dissipativos. Além disso, os hamiltonianos não-hermitianos com simetria ininterrupta de tempo de paridade (PT) têm todos os autovalores reais. Os hamiltonianos não-hermitianos surgem naturalmente em sistemas quânticos como interações efetivas para um subsistema. Esses hamiltonianos podem ser propostos fenomenologicamente ou podem ser encontrados exatamente ou aproximadamente, aplicando a técnica de projeção de Feshbach para descrever a dinâmica no subsistema. (pt) |
dbo:wikiPageID | 51614413 (xsd:integer) |
dbo:wikiPageLength | 10193 (xsd:nonNegativeInteger) |
dbo:wikiPageRevisionID | 1114396537 (xsd:integer) |
dbo:wikiPageWikiLink | dbr:Carl_M._Bender dbr:Quantum_mechanics dbr:Metamaterial dbr:Norm_(mathematics) dbr:Classical_mechanics dbc:Quantum_optics dbr:Eigenfunction dbr:Hamiltonian_(quantum_mechanics) dbr:Physical_Review_Letters dbr:T-symmetry dbr:Time_evolution dbr:Dannie_Heineman_Prize_for_Mathematical_Physics dbr:Hilbert–Pólya_conjecture dbr:Dorje_C._Brody dbr:Inner_product_space dbr:Nuclear_magnetic_resonance dbr:Hermitian_operator dbr:Electric_circuit dbr:Ali_Mostafazadeh dbr:Parity_inversion dbr:Pseudo-Hermitian |
dbp:wikiPageUsesTemplate | dbt:Reflist dbt:Short_description dbt:Technical |
dcterms:subject | dbc:Quantum_optics |
rdfs:comment | PT symmetry was initially studied as a specific system in non-Hermitian quantum mechanics, where Hamiltonians are not Hermitian. In 1998, physicist Carl Bender and former graduate student Stefan Boettcher published in Physical Review Letters a paper in quantum mechanics, "Real Spectra in non-Hermitian Hamiltonians Having PT Symmetry." In this paper, the authors found non-Hermitian Hamiltonians endowed with an unbroken PT symmetry (invariance with respect to the simultaneous action of the parity-inversion and time reversal symmetry operators) also may possess a real spectrum. Under a correctly-defined inner product, a PT-symmetric Hamiltonian's eigenfunctions have positive norms and exhibit unitary time evolution, requirements for quantum theories. Bender won the 2017 Dannie Heineman Prize (en) A mecânica quântica não-hermitiana é uma mecânica quântica que pode ser construída sobre um hamiltoniano complexo que não é hermitiano, mas que satisfaz a condição física da simetria de reflexão espaço-tempo. A mecânica quântica não-hermitiana aparece no estudo de sistemas dissipativos. Além disso, os hamiltonianos não-hermitianos com simetria ininterrupta de tempo de paridade (PT) têm todos os autovalores reais. (pt) |
rdfs:label | Non-Hermitian quantum mechanics (en) Mecânica quântica não-hermitiana (pt) |
owl:sameAs | wikidata:Non-Hermitian quantum mechanics dbpedia-pt:Non-Hermitian quantum mechanics https://global.dbpedia.org/id/2e9k2 |
prov:wasDerivedFrom | wikipedia-en:Non-Hermitian_quantum_mechanics?oldid=1114396537&ns=0 |
foaf:isPrimaryTopicOf | wikipedia-en:Non-Hermitian_quantum_mechanics |
is dbo:knownFor of | dbr:Carl_M._Bender |
is dbo:wikiPageRedirects of | dbr:Non-Hermitian_Quantum_Mechanics dbr:PT_symmetry dbr:Parity-time_symmetry |
is dbo:wikiPageWikiLink of | dbr:Carl_M._Bender dbr:Avadh_Saxena dbr:Symmetry_in_quantum_mechanics dbr:Hermitian_function dbr:Dorje_C._Brody dbr:Self-adjoint_operator dbr:Non-Hermitian_Quantum_Mechanics dbr:List_of_things_named_after_Charles_Hermite dbr:Eva-Maria_Graefe dbr:Exceptional_point dbr:Nanolaser dbr:PT_symmetry dbr:Parity-time_symmetry |
is dbp:knownFor of | dbr:Carl_M._Bender |
is foaf:primaryTopic of | wikipedia-en:Non-Hermitian_quantum_mechanics |