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Range, μSv/h Range, μR/h Measurement time, seconds Measuring of beta and gamma radiation and range of energy PC link Extra features SA-05A [1] Switzerland: 119x65x26.5 135 Built-in lithium polymer battery LCD No No Geiger–Müller tube LND 713 0.01–6000 No 1–60 0.05–1.3 MeV USB: Clock, calendar and data logger ANRI 01-02 Sosna [2 ...
In this case, reaction of hexahedral silsesquioxane and CF 3 SO 3 H in DMSO conducted in 1 : 12 molar ratio gives heptahedral silsesquioxane. In the first step CF 3 SO 3 H acid attacks siloxane Si-O-Si bonds and the formation of Si-O-SO 2 CF 3 bond parallel with cage opening process is observed and compound B is obtained (Figure below). Such an ...
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Polarization gradient cooling (PG cooling), or Sisyphus cooling, is a technique in laser cooling of atoms by dampening the motion of the trapped particles via photon momentum. It was proposed to explain the experimental observation of cooling below the Doppler limit [ 1 ] observed in cesium atom-related laser cooling experiments in 1985.
C L is the corrected length of the line to be measured or laid out; M L is the measured length or length to be laid out; N L is the nominal length of the tape as specified by its mark; K L is a known length; Corr is the ratio of measured to actual length , determined by measuring a known length.
Flux F through a surface, dS is the differential vector area element, n is the unit normal to the surface. Left: No flux passes in the surface, the maximum amount flows normal to the surface. Right: The reduction in flux passing through a surface can be visualized by reduction in F or d S equivalently (resolved into components , θ is angle to ...
Schematic for blind FROG implemented in polarization-gate (PG) geometry. If Pulse #2 is equal to Pulse #1, this is the PG FROG beam geometry, and if Pulse #2 is known, this is the PG XFROG beam geometry. Double-blind frequency-resolved optical gating (double-blind FROG) is a method for simultaneously measuring two unknown ultrashort laser pulses.
The post-measurement state is not determined by the POVM itself, but rather by the PVM that physically realizes it. Since there are infinitely many different PVMs that realize the same POVM, the operators { F i } i = 1 n {\displaystyle \{F_{i}\}_{i=1}^{n}} alone do not determine what the post-measurement state will be.