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1  uptake and storage of anthropogenic carbon (Cant).
2 he Bose factor around T(CDW), and peaks at T(Canting).
3 low for the design of the track's radius and cant.
4 ow that the mechanism is enabled by the spin canting.
5                           Cross-links have R canting (3'-G* H8 atom toward 5'-G*) in duplexes and L c
6 '-G* H8 atom toward 5'-G*) in duplexes and L canting (5'-G* H8 atom toward 3'-G*) in ss models.
7  a c-axis double cone AFM structure around T(Canting) ~ 60 K.
8 ization, suggesting it still keeps the small canted AFM state.
9 ith Chern number C = 1 appears as the AFM to canted-AFM phase transition happens.
10 p forms a H-bond to HN-Pt (indicating that R canting allows H-bonding).
11 trafast damping results in an immediate spin canting along the short precession axis.
12 red (64)Cu retention in vitro and in vivo in CaNT and EMT6 cells or cancers after the administration
13                                    Following Cant and Goodale (2007), we investigate whether the LOC
14 ure, focusing on the combined effects of the cant and varying train speeds.
15  interplay of inter-layer interactions, spin canting and chemical disorder stabilizes this state.
16 ructure of FeGe at temperatures well above T(Canting) and T(CDW) that merge into gapped commensurate
17 ariables such as radius, lateral resistance, cant, and initial misalignment were incorporated to comp
18 louds was observed twice; its brightness and cant angle evolved in a manner consistent with this hypo
19 sults demonstrate that variations in winglet cant angle significantly alter the distribution of [Form
20 pan, particularly near the wingtip, and that cant angle strongly impacts overall performance, at time
21 hortcoming two sensors were assembled with a canted angle similar to that employed in radar bearing l
22 age (+/-60 degrees ) based on the 30 degrees canted angle used.
23 hese switching phenomena can be tuned by the canting angle and the in-plane external field.
24                                            A canting angle of 0.08 degrees was estimated from M vs H
25 emnant magnetization of 10 emu.Oe/mol, and a canting angle of 0.5 degrees .
26 a spin-canted antiferromagnet at 8 K, with a canting angle phi = 0.14 degrees and a coercive field H(
27 ng is driven by a quantitative change in the canting angle rather than a change in the ground state s
28  see text]) and APL distributions at various cant angles near the wingtip and root areas.
29 is study investigates the effects of winglet cant angles on both the aerodynamics and aeroacoustics o
30 of electronic states with different relative canting angles.
31 ndent T(N) and resistivity enhancement, spin-canting, anisotropy reduction, dynamic polarization hyst
32 c interactions led to magnetic ordering as a canted antiferromagnet (T(N) = 3.8 K) with a small spont
33  The unsolvated material 3a orders as a spin-canted antiferromagnet at 8 K, with a canting angle phi
34                      This material is a spin canted antiferromagnet below 15.9 K with a weak ferromag
35 ization data, and a magnetic transition to a canted antiferromagnet state was found at 24.1 K.
36 pi-stacks, and the material orders as a spin-canted antiferromagnet with T(N) = 35 K, with a spontane
37 ) magnetically orders as a weak ferromagnet (canted antiferromagnet) below 21.0 +/- 0.1 K, as observe
38 rough three ordered phases: antiferromagnet, canted antiferromagnet, and ferromagnet.
39 y induced magnetic state resembles that of a canted antiferromagnet, opening an avenue toward creatin
40 thoferrite, YFeO(3), a perovskite-structured canted antiferromagnet.
41                            This results in a canted antiferromagnetic arrangement in which the domina
42      Here we demonstrate experimentally that canted antiferromagnetic BaMnSb2 is a 3D Weyl semimetal
43 ographic axis giving a quasi-one-dimensional canted antiferromagnetic character, as shown by magnetic
44 ffraction near the Dy L(3) edge, we unveil a canted antiferromagnetic ground state arising from a qua
45 al phase is significantly enhanced above the canted antiferromagnetic moment in the bulk phase, as a
46 y functional theory calculations reveals the canted antiferromagnetic nature with significant spin fl
47 omagnetic order for 304 K < T < 565 K, but a canted antiferromagnetic order with a ferromagnetic comp
48 magnetic structure of ferromagnetic and spin-canted antiferromagnetic ordered materials as well as an
49         A weak ferromagnetic transition with canted antiferromagnetic spins along the a-axis is found
50                                It exhibits a canted antiferromagnetic state below 35 kelvin, with mag
51                             In the resulting canted antiferromagnetic state, we observe transport sig
52  the Mn(2+) centres in MnSrTa(2)O(7) adopt a canted antiferromagnetic state, with a small spontaneous
53 e, the magnetic state of Eu evolves from the canted antiferromagnetic structure in the ground state,
54 adratic) manner in the antiferroquadrupolar (canted antiferromagnetic) phase, which are attributed to
55  minority spin states of ferromagnetic, spin-canted antiferromagnetic, and fully antiferromagnetic bi
56 i(2)Te(4) is a rare platform for realizing a canted-antiferromagnetic (cAFM) Chern insulator with ele
57 ing below 50 K, Sr(3)Co(2)O(4)Cl(2) adopts a canted antiferromagnetically ordered state.
58 ingle-chain magnet behavior hidden below the canted antiferromagnetism (T(N) = 5.8 K) already evidenc
59 d magneto-optical microscopy measurements by canted antiferromagnetism and find a number of Weyl poin
60 rial that exhibits both ferroelectricity and canted antiferromagnetism at room temperature, making it
61 surements reveal that this material exhibits canted antiferromagnetism below 15.5 K.
62  ordering (the cluster glassy state) and the canted antiferromagnetism, and then the direct interacti
63                                          The canted antiferromagnets combine antiferromagnetic order
64  (that is, all of the effects present in the canted antiferromagnets(11,12)).
65                                    A signifi-cant association was observed between variations in two
66 in which Delta-Rh intercalates in one of two canted binding conformations.
67 hange and magnetic anisotropy amplifies this canting by several orders of magnitude towards large-amp
68                      The observation of spin-canting can only be understood in terms of multiorbital
69 hyper-/hypo-methylated sequences where signi.cant changes in methylation levels were observed in drug
70 rically with each other and together adopt a canted conformation relative to the catalytic domains.
71 g and form compressive strain-induced c-axis canting defects, while Nd(4)Ni(3)O(8) films on NdGaO(3)
72                                   Hence, the canted directionality of the squaramide (NH)2 motif, fav
73 antiferromagnetic Mn(2+) spin ordering which cants Fe(3+) and Re(5+) spins and reduces spin-polarizat
74                          Here we show that a canted ferromagnetic phase which is preceded by local po
75  Commensurate antiferromagnetic layers and a canted ferromagnetic structure dominate the Si-rich part
76  in the lattice could lead to the local spin canting for a toroidal moment along the c axis.
77 he first examples of an HH1 conformer with R canting for ss oligos longer than d(GpG) (Bip = 2,2'-bip
78 plex spin-orbit torque switching observed in canted Gd(x)Co(100-x) not only provides a platform for s
79 3 manifest a distortion in which one smif is canted in the plane perpendicular to the other.
80 steric effect of the 5'-group, favoring left canting in cisplatin-DNA adducts.
81 .I-1c-treated pigs also exhibited a signi fi cant increase in left atrial ejection fraction at 2 mont
82       In these, the 5'-T residue decreases R canting (indicating steric clashes with the 5'-G*) and t
83                                Johnstone and Cant introduce menopause and the phenomenon of an extend
84            However, almost 2/3 of the excess Cant is stored below the thermocline.
85 logical spin glass and (2) a frustrated spin-canted magnet with low-temperature exchange bias.
86 tahedral tilting, with local distortions and canted magnetic Ce(3+) order evidencing two-dimensional
87 predicted that the in-plane component of the canted magnetic moment at the CoFe/BiFeO3 interface can
88 etic anisotropy, Neel vector orientation and canted magnetism via electron injection and local distor
89 ic order under ambient conditions via a spin canting mechanism, with Tc controlled by the strength of
90     Pseudodipolar interactions lead to a net canted moment along the c-axis, while the sublattice mag
91 ield through a ~180 degrees switching of the canted moment in BiFeO3.
92 f the magnetization in the CoFe layer to the canted moment in the BiFeO3 layer.
93  deterministic reversal of the DM vector and canted moment using an electric field at room temperatur
94 magnet with T(N) = 35 K, with a spontaneous (canted) moment M(spont) = 1.4 x 10(-3) muB and a coerciv
95 two MOFs, NipymcaCl and NipymcaBr, featuring canted Ni(2+)-based moments.
96                            Almost 2/3 of the Cant ocean uptake enters via gas exchange in waters that
97 thin FeMoco alters this BS state by a slight canting of spins and is analogous in several respects to
98      Its weak ferromagnetism arises from the canting of the antiferromagnetically aligned spins by th
99  enhances polarization switching and permits canting of the ordered magnetic moments.
100 ibility of changing the magnitude and/or the canting of the organic molecular dipole opens new routes
101  a strong spin-orbit coupling and results in canting of the spins, thereby producing net magnetizatio
102                      In vivo in mice bearing CaNT or EMT6 tumors, biodistributions and dynamic PET da
103 multiple copies of an Rta DNA motif (called "CANT" or Rta-c) proximal to an RBP-Jkappa motif.
104 etic correlations, a precursor to long-range canted order.
105 ivity(15), in which fluctuations in the spin-canting order contribute to the pairing interaction.
106                                   A peculiar canted ordering of the organic A-cation dipole moments g
107 grown on the topological insulator Bi2Te3 is canted out of the high-symmetry directions of the surfac
108 ce this interaction has to facilitate higher canting per spin to complete a 360 rotation along the di
109 colloidal silica superballs crystallize into canted phases in the presence of depletants.
110  and strain control of the out-of-plane spin-canting process.
111             We have termed this element the "CANT repeat." CANT repeats are found on both strands of
112  have termed this element the "CANT repeat." CANT repeats are found on both strands of DNA and have a
113                                The number of CANT repeats, their presence in palindromes, and their p
114 these water masses essentially form a common Cant reservoir.
115 ounterparts, the oxidized cluster has a spin-canted, S = (1)/(2) ground state, and the reduced cluste
116 rings of PIN-acac complexes 18a and 18b were canted significantly from planarity and projected the im
117 cited in a broad class of iron oxides with a canted spin configuration.
118 omena, we demonstrate a new functionality of canted spin order for magnonics and show that it facilit
119                     Interestingly, different canting spin stripes along three 120 degree propagation
120 omly in a magnetic phase, attesting that the canting spin stripes are three-fold degenerate states ak
121 es akin to helices and the multiple state of canting spin stripes is a circular configuration with ze
122 romagnetic one, a magnetic phase composed of canting spin stripes, never observed in the chiral magne
123 tivity straddles a transition between a spin-canted state with a finite in-plane magnetic moment and
124                                  In the spin-canting state, another resonance occurs at 10.5 tesla fr
125 o-solid phase transitions between square and canted structures.
126  effects can be traced to a large anistropic canting, that can be engineered into the Gd(x)Co(100-x)
127 d zero-dimensional molecule to ordered, spin-canted, three-dimensional lattice being the result of th
128                That in vivo, in the EMT6 and CaNT tumors studied, the distribution of radiocopper fro
129 ith 64 bp of the Mta promoter but not single CANT units.
130     On further cooling, the compounds become canted weak ferromagnets below 40 K.
131 e vaginal lumen and penis tip were both left-canted with similar angular bends that mirrored one anot
132  topological AHE due to an out-of-plane spin canting with respect to the Kagome plane.
133 were carried out using a murine tumor model (CaNT) with single administration of a dose well below th
134 f an out of plane moment developed from spin canting within Fe3(mu-OH)3 triangles.

 
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