ライフサイエンスコーパス: cant

1 uptake and storage of anthropogenic carbon (Cant).

2 Cross-links have R canting (3'-G* H8 atom toward 5'-G*) in duplexes and L c

3 '-G* H8 atom toward 5'-G*) in duplexes and L canting (5'-G* H8 atom toward 3'-G*) in ss models.

4 ization, suggesting it still keeps the small canted AFM state.

5 p forms a H-bond to HN-Pt (indicating that R canting allows H-bonding).

6 red (64)Cu retention in vitro and in vivo in CaNT and EMT6 cells or cancers after the administration

7 Following Cant and Goodale (2007), we investigate whether the LOC

8 interplay of inter-layer interactions, spin canting and chemical disorder stabilizes this state.

9 louds was observed twice; its brightness and cant angle evolved in a manner consistent with this hypo

10 hortcoming two sensors were assembled with a canted angle similar to that employed in radar bearing l

11 age (+/-60 degrees ) based on the 30 degrees canted angle used.

12 emnant magnetization of 10 emu.Oe/mol, and a canting angle of 0.5 degrees .

13 a spin-canted antiferromagnet at 8 K, with a canting angle phi = 0.14 degrees and a coercive field H(

14 of electronic states with different relative canting angles.

15 The unsolvated material 3a orders as a spin-canted antiferromagnet at 8 K, with a canting angle phi

16 This material is a spin canted antiferromagnet below 15.9 K with a weak ferromag

17 pi-stacks, and the material orders as a spin-canted antiferromagnet with T(N) = 35 K, with a spontane

18 ) magnetically orders as a weak ferromagnet (canted antiferromagnet) below 21.0 +/- 0.1 K, as observe

19 This results in a canted antiferromagnetic arrangement in which the domina

20 Here we demonstrate experimentally that canted antiferromagnetic BaMnSb2 is a 3D Weyl semimetal

21 al phase is significantly enhanced above the canted antiferromagnetic moment in the bulk phase, as a

22 y functional theory calculations reveals the canted antiferromagnetic nature with significant spin fl

23 omagnetic order for 304 K < T < 565 K, but a canted antiferromagnetic order with a ferromagnetic comp

24 magnetic structure of ferromagnetic and spin-canted antiferromagnetic ordered materials as well as an

25 In the resulting canted antiferromagnetic state, we observe transport sig

26 e, the magnetic state of Eu evolves from the canted antiferromagnetic structure in the ground state,

27 minority spin states of ferromagnetic, spin-canted antiferromagnetic, and fully antiferromagnetic bi

28 ing below 50 K, Sr(3)Co(2)O(4)Cl(2) adopts a canted antiferromagnetically ordered state.

29 ordering (the cluster glassy state) and the canted antiferromagnetism, and then the direct interacti

30 A signifi-cant association was observed between variations in two

31 in which Delta-Rh intercalates in one of two canted binding conformations.

32 The observation of spin-canting can only be understood in terms of multiorbital

33 hyper-/hypo-methylated sequences where signi.cant changes in methylation levels were observed in drug

34 rically with each other and together adopt a canted conformation relative to the catalytic domains.

35 Hence, the canted directionality of the squaramide (NH)2 motif, fav

36 antiferromagnetic Mn(2+) spin ordering which cants Fe(3+) and Re(5+) spins and reduces spin-polarizat

37 Here we show that a canted ferromagnetic phase which is preceded by local po

38 he first examples of an HH1 conformer with R canting for ss oligos longer than d(GpG) (Bip = 2,2'-bip

39 3 manifest a distortion in which one smif is canted in the plane perpendicular to the other.

40 steric effect of the 5'-group, favoring left canting in cisplatin-DNA adducts.

41 .I-1c-treated pigs also exhibited a signi fi cant increase in left atrial ejection fraction at 2 mont

42 In these, the 5'-T residue decreases R canting (indicating steric clashes with the 5'-G*) and t

43 However, almost 2/3 of the excess Cant is stored below the thermocline.

44 predicted that the in-plane component of the canted magnetic moment at the CoFe/BiFeO3 interface can

45 ic order under ambient conditions via a spin canting mechanism, with Tc controlled by the strength of

46 Pseudodipolar interactions lead to a net canted moment along the c-axis, while the sublattice mag

47 ield through a ~180 degrees switching of the canted moment in BiFeO3.

48 f the magnetization in the CoFe layer to the canted moment in the BiFeO3 layer.

49 deterministic reversal of the DM vector and canted moment using an electric field at room temperatur

50 magnet with T(N) = 35 K, with a spontaneous (canted) moment M(spont) = 1.4 x 10(-3) muB and a coerciv

51 Almost 2/3 of the Cant ocean uptake enters via gas exchange in waters that

52 thin FeMoco alters this BS state by a slight canting of spins and is analogous in several respects to

53 Its weak ferromagnetism arises from the canting of the antiferromagnetically aligned spins by th

54 enhances polarization switching and permits canting of the ordered magnetic moments.

55 ibility of changing the magnitude and/or the canting of the organic molecular dipole opens new routes

56 In vivo in mice bearing CaNT or EMT6 tumors, biodistributions and dynamic PET da

57 etic correlations, a precursor to long-range canted order.

58 A peculiar canted ordering of the organic A-cation dipole moments g

59 grown on the topological insulator Bi2Te3 is canted out of the high-symmetry directions of the surfac

60 colloidal silica superballs crystallize into canted phases in the presence of depletants.

61 We have termed this element the "CANT repeat." CANT repeats are found on both strands of

62 have termed this element the "CANT repeat." CANT repeats are found on both strands of DNA and have a

63 The number of CANT repeats, their presence in palindromes, and their p

64 these water masses essentially form a common Cant reservoir.

65 rings of PIN-acac complexes 18a and 18b were canted significantly from planarity and projected the im

66 cited in a broad class of iron oxides with a canted spin configuration.

67 Interestingly, different canting spin stripes along three 120 degree propagation

68 omly in a magnetic phase, attesting that the canting spin stripes are three-fold degenerate states ak

69 es akin to helices and the multiple state of canting spin stripes is a circular configuration with ze

70 romagnetic one, a magnetic phase composed of canting spin stripes, never observed in the chiral magne

71 o-solid phase transitions between square and canted structures.

72 d zero-dimensional molecule to ordered, spin-canted, three-dimensional lattice being the result of th

73 That in vivo, in the EMT6 and CaNT tumors studied, the distribution of radiocopper fro

74 ith 64 bp of the Mta promoter but not single CANT units.

75 On further cooling, the compounds become canted weak ferromagnets below 40 K.

76 were carried out using a murine tumor model (CaNT) with single administration of a dose well below th

77 f an out of plane moment developed from spin canting within Fe3(mu-OH)3 triangles.