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Single channel detection

Figure 1.33 The underlying principle of the Redfield technique. Complex Fourier transformation and single-channel detection gives spectrum (a), which contains both positive and negative frequencies. These are shown separately in (b), corresponding to the positive and negative single-quantum coherences. The overlap disappears when the receiver rotates at a frequency that corresponds to half the sweep width (SW) in the rotating frame, as shown in (c). After a real Fourier transformation (involving folding about n = 0), the spectrum (d) obtained contains only the positive frequencies. Figure 1.33 The underlying principle of the Redfield technique. Complex Fourier transformation and single-channel detection gives spectrum (a), which contains both positive and negative frequencies. These are shown separately in (b), corresponding to the positive and negative single-quantum coherences. The overlap disappears when the receiver rotates at a frequency that corresponds to half the sweep width (SW) in the rotating frame, as shown in (c). After a real Fourier transformation (involving folding about n = 0), the spectrum (d) obtained contains only the positive frequencies.
In quadrature detection, the transmitter offset frequency is posidoned at the center of the F domain (i.e., at F2 = 0 in single-channel detection it is positioned at the left edge). Frequencies to the left (or downfield) of the transmitter offset frequency are positive those to the right (or upheld) of it are negative. [Pg.158]

The main problem has been a methodological one. The patch clamp analysis of single channels views the world of channels through a very small analytical window [10]. A single channel event (opening) needs to be sufficiently long-lived and sufficiently large to be picked up within the current noise band under optimized conditions, and with the low-pass filter set to say 2 kHz. The open time needs to be close to a millisecond and the current amplitude close to 0.5 pA to permit detection. [Pg.277]

GL 3] [GL 4] [GL 5] [GL 6] [GL 7] [R 5] [P 5] No clear difference in the performance of a single-channel micro reactor and a numbered-up three-channel micro reactor was detected [16]. However, many differences in the results were found which were... [Pg.611]

Implementation of time domain FLIM methods is comparatively straightforward in laser scanning microscopes (LSMs). Here, pointscanning is used so that single channel lifetime detection suffices. In principle, standard fluorescence lifetime detection equipment developed for spectroscopy can be used in combination with point-scanning systems and a pulsed laser. [Pg.117]

A Princeton Gamma Tech Si (Li) solid state detector in conjunction with an EG G Ortec Model 673 Spectroscopy Amplifier and a Tennelec Model 450 Single Channel analyzer were employed to detect the characteristic Ru Ka... [Pg.221]

Section 6.2.2) as follows because the excited-state lifetime is generally of a few nanoseconds, a single-channel analyzer is used in conjunction with a time-to-amplitude converter to process only the photons that are detected at times longer than 1 ns after the excitation pulse. [Pg.374]

A premixture of 8 and soybean lecithin gave stable single channel currents with well-defined transitions between open and closed states with the 0.1-Is time scale. The conductance level detected was 6.1 0.5 pS at 0.5 M KCl solution. At various transmembrane voltages with different molar ratios of 8-to-lipid in the range 1/200 - 1/3000, an identical conductance level was always observed. This observation is therefore compatible with the original idea that monomeric 8 itself defines a pore mouth with a specified diameter in the single lipid layer. It gave a cation/anion... [Pg.179]


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See also in sourсe #XX -- [ Pg.59 ]

See also in sourсe #XX -- [ Pg.46 ]




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