Phys. Rev. Lett. 110, 156402 - Institute for Quantum Optics and
... where D½c ¼ ccy 12 ðcy c þ cy cÞ and the single spin dephasing T21 is assumed to be Markovian for simplicity (see below). Note that we absorbed a shift of =2 into B , and ignored single spin relaxation as T1 can be several minutes at low temperatures [34]. The second line describes collect ...
... where D½c ¼ ccy 12 ðcy c þ cy cÞ and the single spin dephasing T21 is assumed to be Markovian for simplicity (see below). Note that we absorbed a shift of =2 into B , and ignored single spin relaxation as T1 can be several minutes at low temperatures [34]. The second line describes collect ...
Quantum process tomography of two-qubit controlled-Z
... capacitance Cc. The avoided crossing for the two-photon line at ⌬i ⯝ 0.066 gives a splitting of 9.7⫾ 0.2 MHz, about 冑2 / 2 times as large as the main resonance, as expected from a 兩11典 and 兩02典 interaction. The slope of the resonance between the B , as expected for the 兩11典 state. two crossings is 1 ...
... capacitance Cc. The avoided crossing for the two-photon line at ⌬i ⯝ 0.066 gives a splitting of 9.7⫾ 0.2 MHz, about 冑2 / 2 times as large as the main resonance, as expected from a 兩11典 and 兩02典 interaction. The slope of the resonance between the B , as expected for the 兩11典 state. two crossings is 1 ...
Markov chain model in maximum-likelihood sequence detection for
... the fading correlation length 0 and the observation interval 0 is smaller than the fading correlation time 0 . If the receiver has knowledge of the joint temporal statistics of the fading, maximumlikelihood sequence detection (MLSD) can be employed, but at the cost of high computational complexity. ...
... the fading correlation length 0 and the observation interval 0 is smaller than the fading correlation time 0 . If the receiver has knowledge of the joint temporal statistics of the fading, maximumlikelihood sequence detection (MLSD) can be employed, but at the cost of high computational complexity. ...
Electrical properties of Nb-doped titanium dioxide TiO at room temperature A.
... with CuKα filtered radiation in the 2θ range from 10º to 80º. Phase identification was performed using the data base ICDD. The analysis revealed that the samples containing 10 at. % of Nb and less are homogeneous and crystallize in the rutile phase. On the other hand, apart rutile phase, the traces ...
... with CuKα filtered radiation in the 2θ range from 10º to 80º. Phase identification was performed using the data base ICDD. The analysis revealed that the samples containing 10 at. % of Nb and less are homogeneous and crystallize in the rutile phase. On the other hand, apart rutile phase, the traces ...
the_nature_of_covalent_bonding
... may form double or triple bonds if there is an abundance of single e Two shared pairs = double covalent bond Three shared pairs = triple covalent bond Some ...
... may form double or triple bonds if there is an abundance of single e Two shared pairs = double covalent bond Three shared pairs = triple covalent bond Some ...
Evidence from the Absorption and Emission Spectra
... (Matheson, Coleman and Bell) and were used without further purification. 2a and 2b were synthesized according to published procedures.6c.d 2b was sublimed immediately before use. Electronic Absorption and ESR Spectroscopy. Photolysis (254 nm) of 2a in glassy matrices (MP, EPA, MCH, I-P-2-P) at tempe ...
... (Matheson, Coleman and Bell) and were used without further purification. 2a and 2b were synthesized according to published procedures.6c.d 2b was sublimed immediately before use. Electronic Absorption and ESR Spectroscopy. Photolysis (254 nm) of 2a in glassy matrices (MP, EPA, MCH, I-P-2-P) at tempe ...
Ramsey Interference in One-Dimensional Systems: The Full
... many-body origin of Ramsey fringe decay. In the following, we argue that unambiguous signatures of the multimode decoherence are found in the full distribution function of the Ramsey fringe amplitudes. Such distribution functions should be accessible in experiments with 1D quasicondensates realized ...
... many-body origin of Ramsey fringe decay. In the following, we argue that unambiguous signatures of the multimode decoherence are found in the full distribution function of the Ramsey fringe amplitudes. Such distribution functions should be accessible in experiments with 1D quasicondensates realized ...
Phys. Rev. Lett. 102, 223901 (2009)
... tion in the fluorescence signal (even for long measurement times) and the short loading time of <1 s. The modes from a frequency comb can be described by the repetition frequency frep of the pulses and a carrierenvelope offset frequency fceo . The frequency of the nth mode is equal to fn ¼ fceo þ n ...
... tion in the fluorescence signal (even for long measurement times) and the short loading time of <1 s. The modes from a frequency comb can be described by the repetition frequency frep of the pulses and a carrierenvelope offset frequency fceo . The frequency of the nth mode is equal to fn ¼ fceo þ n ...
