arXiv:1501.06883v1 [nucl
... whereby each point of the movement space of the scanner can be defined by a unique set of scale factors. Featureoriented scanning (FOS) methodology is used to implement the distributed calibration, which permits to exclude in situ the negative influence of thermal drift, creep and hysteresis on the ...
... whereby each point of the movement space of the scanner can be defined by a unique set of scale factors. Featureoriented scanning (FOS) methodology is used to implement the distributed calibration, which permits to exclude in situ the negative influence of thermal drift, creep and hysteresis on the ...
![arXiv:1501.01596v1 [cond-mat.mtrl-sci] 3 Jan 2015](http://s1.studyres.com/store/data/008057215_1-2593210d98eafff454da21c3b7b4536e-300x300.png)
arXiv:1501.01596v1 [cond-mat.mtrl-sci] 3 Jan 2015
... level with a good selection of radiopure materials; and a high signal-to-noise ratio due to its low capacitance, which is proportional to the radius of the central electrode and does not depend on the vessel size. Indeed, previous works have shown that an energy threshold as low as 100 eV [4, 5] is ...
... level with a good selection of radiopure materials; and a high signal-to-noise ratio due to its low capacitance, which is proportional to the radius of the central electrode and does not depend on the vessel size. Indeed, previous works have shown that an energy threshold as low as 100 eV [4, 5] is ...
Asymptotic Equivalence of KMS States in Rindler spacetime
... Consider the translates O + x (s) and the corresponding local field algebra A(O + x (s)) of a massless scalar field. Then for all β1 , β2 > 0 ...
... Consider the translates O + x (s) and the corresponding local field algebra A(O + x (s)) of a massless scalar field. Then for all β1 , β2 > 0 ...
quant-ph/0204033 PDF
... physical laws contains two mutually exclusive values: attachment space attaching to object and detachment space detaching from object. However, the cosmic physical system could not start with mutually exclusive attachment space and detachment space at the same time in the beginning. The way out of t ...
... physical laws contains two mutually exclusive values: attachment space attaching to object and detachment space detaching from object. However, the cosmic physical system could not start with mutually exclusive attachment space and detachment space at the same time in the beginning. The way out of t ...
PPT - Fernando Brandao
... The main idea is to connect the convertibility of resource states to the distinguishability of resource states from nonresource ones Basically, if a resource theory is such that we can distinguish, by measurements, many copies of a resource state from nonresource states pretty well, then the the ...
... The main idea is to connect the convertibility of resource states to the distinguishability of resource states from nonresource ones Basically, if a resource theory is such that we can distinguish, by measurements, many copies of a resource state from nonresource states pretty well, then the the ...
Error Free Quantum Reading by Quasi Bell State of Entangled
... The main purpose of the quantum information science is to overcome performances of the classical information technology. Hence, when one considers subjects for quantum information science, the problems that classical information technology cannot cope with has to be chosen. For instance, the quantum ...
... The main purpose of the quantum information science is to overcome performances of the classical information technology. Hence, when one considers subjects for quantum information science, the problems that classical information technology cannot cope with has to be chosen. For instance, the quantum ...
Williams
... Si sphere mass can be measured in vacuum or in air (buoyancy correction required – but the density and volume are known very well) Determining NA was much harder then realizing mass with the sphere ...
... Si sphere mass can be measured in vacuum or in air (buoyancy correction required – but the density and volume are known very well) Determining NA was much harder then realizing mass with the sphere ...
Second quantization of the elliptic Calogero
... we will construct regularized anyons φε (x) which for ε > 0 can be multiplied without ambiguities and obey Eq. (1) only in the limit ε ↓ 0. We perform that latter limit at a later point where it can be taken without difficulty.5 For simplicity, we will regard all quantum fields only as sesquilinear ...
... we will construct regularized anyons φε (x) which for ε > 0 can be multiplied without ambiguities and obey Eq. (1) only in the limit ε ↓ 0. We perform that latter limit at a later point where it can be taken without difficulty.5 For simplicity, we will regard all quantum fields only as sesquilinear ...
Thesis - Archive ouverte UNIGE
... confronted with experiment, using standard and adapted post-Newtonian (PN) tools. The laboratory is provided by the Solar System, binary pulsars and future detections at gravitational wave observatories. We test Horava gravity by studying emission of gravitational radiation in the weak-field limit f ...
... confronted with experiment, using standard and adapted post-Newtonian (PN) tools. The laboratory is provided by the Solar System, binary pulsars and future detections at gravitational wave observatories. We test Horava gravity by studying emission of gravitational radiation in the weak-field limit f ...
Lecture Notes
... • Coherent states are readily available from a laser. No nonclassical light needed ...
... • Coherent states are readily available from a laser. No nonclassical light needed ...
Primitive ontology and quantum state in the GRW matter density theory
... dq1 · · · dqN δ(qi − x) |ψ(q1 , . . . , qN , t)| ...
... dq1 · · · dqN δ(qi − x) |ψ(q1 , . . . , qN , t)| ...
Fractals and Dimension
... with the properties that the fi all have the same contraction ratio λ, and the fi (S) do not overlap (if at worst they meet at their edges) then we can use a box counting argument to deduce that the dimension of S is ln(m)/ ln(1/λ), where m is the number of maps in the IFS. If we have a picture whic ...
... with the properties that the fi all have the same contraction ratio λ, and the fi (S) do not overlap (if at worst they meet at their edges) then we can use a box counting argument to deduce that the dimension of S is ln(m)/ ln(1/λ), where m is the number of maps in the IFS. If we have a picture whic ...
Document
... Masses higher than 1700 MeV, width ~ hundreds MeV Mass of the pentaquark is roughly 5 M +(strangeness) ~ 1800 MeV An additional q –anti-q pair is added as constituent ...
... Masses higher than 1700 MeV, width ~ hundreds MeV Mass of the pentaquark is roughly 5 M +(strangeness) ~ 1800 MeV An additional q –anti-q pair is added as constituent ...