Semiclassical Length Measure from a Quantum-Gravity Wave Function
The definition of a length operator in quantum cosmology is usually influenced by a quantum theory for gravity considered. The semiclassical limit at the Planck age must meet the requirements implied in present observations. The features of a semiclassical wave-functional state are investigated, for...
Main Author: | |
---|---|
Format: | Article |
Language: | English |
Published: |
MDPI AG
2017-09-01
|
Series: | Technologies |
Subjects: | |
Online Access: | https://www.mdpi.com/2227-7080/5/3/56 |
id |
doaj-fc006cd06a2a47d3a511af703a2f4b15 |
---|---|
record_format |
Article |
spelling |
doaj-fc006cd06a2a47d3a511af703a2f4b152020-11-25T00:33:39ZengMDPI AGTechnologies2227-70802017-09-01535610.3390/technologies5030056technologies5030056Semiclassical Length Measure from a Quantum-Gravity Wave FunctionOrchidea Maria Lecian0DIAEE—Department for Astronautics Engineering, Electrical and Energetics, Sapienza University of Rome, Via Eudossiana, 18, 00184 Rome, ItalyThe definition of a length operator in quantum cosmology is usually influenced by a quantum theory for gravity considered. The semiclassical limit at the Planck age must meet the requirements implied in present observations. The features of a semiclassical wave-functional state are investigated, for which the modern measure(ment)s is consistent. The results of a length measurement at present times are compared with the same measurement operation at cosmological times. By this measure, it is possible to discriminate, within the same Planck-length expansion, the corrections to a Minkowski flat space possibly due to classicalization of quantum phenomena at the Planck time and those due to possible quantum-gravitational manifestations of present times. This analysis and the comparison with the previous literature can be framed as a test for the verification of the time at which anomalies at present related to the gravitational field, and, in particular, whether they are ascribed to the classicalization epoch. Indeed, it allows to discriminate not only within the possible quantum features of the quasi (Minkowski) flat spacetime, but also from (possibly Lorentz violating) phenomena detectable at high-energy astrophysical scales. The results of two different (coordinate) length measures have been compared both at cosmological time and as a perturbation element on flat Minkowski spacetime. The differences for the components of the corresponding classical(ized) metric tensor have been analyzed at different orders of expansions. The results of the expectation values of a length operator in the universe at the Planck time must be comparable with the same length measurements at present times, as far as the metric tensor is concerned. The comparison of the results of (straight) length measures in two different directions, in particular, can encode the pertinent information about the parameters defining the semiclassical wavefunctional for (semiclassicalized) gravitational field.https://www.mdpi.com/2227-7080/5/3/5604.60.-m quantum gravity03.65.Vf phases: geometricdynamic or topological04.40.Nr Einstein-Maxwell spacetimes, spacetimes with fluids, radiation or classical fields42.50.Xa optical tests of quantum theory04.80.Cc experimental tests of gravitational theories03.65.Sq semiclassical theories and applications98.80.Jk mathematical and relativistic aspects of cosmology98.80.Qc quantum cosmology04. general relativity and gravitation general relativity and gravitation03.65.Ta foundations of quantum mechanics, measurement theory |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Orchidea Maria Lecian |
spellingShingle |
Orchidea Maria Lecian Semiclassical Length Measure from a Quantum-Gravity Wave Function Technologies 04.60.-m quantum gravity 03.65.Vf phases: geometric dynamic or topological 04.40.Nr Einstein-Maxwell spacetimes, spacetimes with fluids, radiation or classical fields 42.50.Xa optical tests of quantum theory 04.80.Cc experimental tests of gravitational theories 03.65.Sq semiclassical theories and applications 98.80.Jk mathematical and relativistic aspects of cosmology 98.80.Qc quantum cosmology 04. general relativity and gravitation general relativity and gravitation 03.65.Ta foundations of quantum mechanics, measurement theory |
author_facet |
Orchidea Maria Lecian |
author_sort |
Orchidea Maria Lecian |
title |
Semiclassical Length Measure from a Quantum-Gravity Wave Function |
title_short |
Semiclassical Length Measure from a Quantum-Gravity Wave Function |
title_full |
Semiclassical Length Measure from a Quantum-Gravity Wave Function |
title_fullStr |
Semiclassical Length Measure from a Quantum-Gravity Wave Function |
title_full_unstemmed |
Semiclassical Length Measure from a Quantum-Gravity Wave Function |
title_sort |
semiclassical length measure from a quantum-gravity wave function |
publisher |
MDPI AG |
series |
Technologies |
issn |
2227-7080 |
publishDate |
2017-09-01 |
description |
The definition of a length operator in quantum cosmology is usually influenced by a quantum theory for gravity considered. The semiclassical limit at the Planck age must meet the requirements implied in present observations. The features of a semiclassical wave-functional state are investigated, for which the modern measure(ment)s is consistent. The results of a length measurement at present times are compared with the same measurement operation at cosmological times. By this measure, it is possible to discriminate, within the same Planck-length expansion, the corrections to a Minkowski flat space possibly due to classicalization of quantum phenomena at the Planck time and those due to possible quantum-gravitational manifestations of present times. This analysis and the comparison with the previous literature can be framed as a test for the verification of the time at which anomalies at present related to the gravitational field, and, in particular, whether they are ascribed to the classicalization epoch. Indeed, it allows to discriminate not only within the possible quantum features of the quasi (Minkowski) flat spacetime, but also from (possibly Lorentz violating) phenomena detectable at high-energy astrophysical scales. The results of two different (coordinate) length measures have been compared both at cosmological time and as a perturbation element on flat Minkowski spacetime. The differences for the components of the corresponding classical(ized) metric tensor have been analyzed at different orders of expansions. The results of the expectation values of a length operator in the universe at the Planck time must be comparable with the same length measurements at present times, as far as the metric tensor is concerned. The comparison of the results of (straight) length measures in two different directions, in particular, can encode the pertinent information about the parameters defining the semiclassical wavefunctional for (semiclassicalized) gravitational field. |
topic |
04.60.-m quantum gravity 03.65.Vf phases: geometric dynamic or topological 04.40.Nr Einstein-Maxwell spacetimes, spacetimes with fluids, radiation or classical fields 42.50.Xa optical tests of quantum theory 04.80.Cc experimental tests of gravitational theories 03.65.Sq semiclassical theories and applications 98.80.Jk mathematical and relativistic aspects of cosmology 98.80.Qc quantum cosmology 04. general relativity and gravitation general relativity and gravitation 03.65.Ta foundations of quantum mechanics, measurement theory |
url |
https://www.mdpi.com/2227-7080/5/3/56 |
work_keys_str_mv |
AT orchideamarialecian semiclassicallengthmeasurefromaquantumgravitywavefunction |
_version_ |
1725315646533664768 |