ライフサイエンスコーパス: bathorhodopsin

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1 found to be very similar to those for squid bathorhodopsin.

2 ation that uncouples the 11H and 12H wags in bathorhodopsin.

3 plays the dominant role in energy storage in bathorhodopsin.

4 served upon the conversion of rhodopsin into bathorhodopsin.

5 cted had the characteristics of a mixture of bathorhodopsin and a blue-shifted intermediate, BSI, whi

6 esonance Raman spectra of octopus rhodopsin, bathorhodopsin, and isorhodopsin at 120 K have been obta

7 ually low compared to those in rhodopsin and bathorhodopsin, and the C=ND stretching mode shifts down

8 an early photointermediate similar to bovine bathorhodopsin (Batho).

9 This situation is resolved in bathorhodopsin, because photoisomerization of the chromo

10 ied except E181D showed accelerated decay of bathorhodopsin compared to wild type.

11 s observed in the absorption spectrum of the bathorhodopsin decay product, BSI.

12 high in the spectra of octopus rhodopsin and bathorhodopsin (> 1200 cm-1) and since the normal mode p

13 ompanying the transformation of rhodopsin to bathorhodopsin have been evaluated.

14 ifts of the primary visual photointermediate bathorhodopsin have been observed by performing double-q

15 s of rhodopsin and its primary photoproduct, bathorhodopsin, have generated structural constraints th

16 te, BSI, which is the first decay product of bathorhodopsin in bovine rhodopsin.

17 inal chromophore during the formation of the bathorhodopsin intermediate (bathoRT) in the room-temper

18 is stabilized and at room temperature where bathorhodopsin is a transient species in the RhRT photos

19 Structure of the squid bathorhodopsin is characterized by formation of a direct

20 The overall yield of bathorhodopsin is improved by using monochromatic 420 nm

21 retinal chromophore at low temperature where bathorhodopsin is stabilized and at room temperature whe

22 phore in the primary photoproduct of vision, bathorhodopsin, is examined to determine the cause of th

23 ionary state mixture is formed consisting of bathorhodopsin (lambda(max) = 545 nm) and isorhodopsin (

24 strate that Glu-181 is negatively charged in bathorhodopsin on the basis of the shift in the batho ab

25 For each mutant, the decay of its bathorhodopsin photoproduct (batho) into an equilibrium

26 ly reveals coherent wavepacket motion in the bathorhodopsin photoproduct over the full vibrational ma

27 light leads to the generation of the active bathorhodopsin photostate in the outer layer of the samp

28 All mutants exhibited bathorhodopsin stability on the 30 ns to 1 micros time s

29 base counterion region in the transition of bathorhodopsin to BSI.

30 se results suggest that the transitions from bathorhodopsin to Lumi and Meta I involve a relaxation o

31 on of the chromophore-protein complex in the bathorhodopsin to Lumi transition thus appears to drive

32 ogen bonding is dramatically weakened in the bathorhodopsin to Lumi transition.

33 diate and to probe structural changes in the bathorhodopsin-to-BSI and BSI-to-lumirhodopsin transitio

34 This result suggests that in the bathorhodopsin-to-BSI transition the highly strained all

35 n the presence of an unrelaxed binding site, bathorhodopsin was found to carry almost 27 kcal/mol ene

36 to longer wavelengths analogous to wild-type bathorhodopsin were seen.

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