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1 ide can be used for passivation of ultrathin black phosphorus.
2 in a single-layer, two-dimensional material, black phosphorus.
3 itting diodes and photodetectors composed of black phosphorus.
4 presence of self-terminated surface bonds in black phosphorus.
5 y interfacing even-layered MnBi(2)Te(4) with black phosphorus.
6 ions donating electrons to surface layers of black phosphorus.
7 ural and electronic relatives alpha-GeSe and black phosphorus.
8 ls, like transition metal dichalcogenides or black phosphorus.
9 ive with atomically thin dichalcogenides and black phosphorus.
10 g graphene, molybdenum disulphide (MoS2) and black phosphorus.
11 o tune the electronic structure of few-layer black phosphorus.
12 ropic layered crystals, such as orthorhombic black-phosphorus.
13 armchair and zigzag crystallographic axes of black-phosphorus.
14  chemical functionalization of 2D exfoliated black phosphorus (2D BP) continues to attract great inte
15  with a tunable, direct bandgap, distinguish black phosphorus 2DEG as a system with unique electronic
16 such as transition-metal dichalcogenides and black phosphorus(6,7).
17                    Here, we create a 2DEG in black phosphorus--a recently added member of the two-dim
18 layed a typical I-V curve similar to that of black phosphorus and a similar mobility reaching 300 cm(
19 der Waals interface of tungsten selenide and black phosphorus and realized in-plane electronic polari
20 ectors based on semiconductors such as PbTe, black phosphorus and tellurene.
21 any layered 2D crystals (including graphene, black phosphorus and versatile metal chalcogenides) can
22 at the interface of a crystalline insulator (black phosphorus) and disordered dopants (alkali metals)
23 materials, transition metal dichalcogenides, black phosphorus, and 2D metal oxides) materials, with t
24 halcogenides, novel van der Waals materials, black phosphorus, and heterostructures.
25 this behaviour is intrinsic for single-layer black phosphorus, and originates from its puckered struc
26  and development of hexagonal boron nitride, black phosphorus, and transition metal disulfides.
27                      Notably, a sulfur-doped black phosphorus anode coupled with a lithium cobalt oxi
28                  Our study paves the way for black phosphorus applications in infrared photonics and
29 substitutional dopants in few-layer and bulk black phosphorus are calculated.
30 rientation-dependent thermal conductivity of black phosphorus are useful for designing devices, as we
31 ndent bandgap tuning properties in intrinsic black phosphorus, arising from the strong interlayer ele
32 is foundational in elucidating the nature of black phosphorus as a ligand and underscores the viabili
33                       We demonstrate printed black phosphorus as a passive switch for ultrafast laser
34 c tensors of Bloch electrons in solids using black phosphorus as a representative material.
35  10 nm thick flake of exfoliated crystalline black phosphorus as an active channel of a field-effect
36 with actively variable spectra by presenting black phosphorus as an ideal candidate.
37 a Sn/SnI4 catalyst mixture has provided bulk black phosphorus at much lower pressures than those requ
38                                              Black phosphorus attracts enormous attention as a promis
39 ccessful synthesis in the bulk form in 1914, black phosphorus (black P) was recently rediscovered fro
40                         We propose the first black phosphorus (BP) - fiber optic biosensor for ultras
41  modify the Lewis basic surface of few-layer black phosphorus (bP) and demonstrate its effectiveness
42 ages over the prototypical 2D Xenes, such as black phosphorus (BP) and graphene.
43                                              Black phosphorus (BP) as a new 2D material has attracted
44                             We report use of black phosphorus (BP) as the active anode for high-rate,
45 hat the inherent Cu(2+)-capturing ability of black phosphorus (BP) can accelerate the degradation of
46 is particularly intriguing in semiconducting black phosphorus (BP) due to the highly anisotropic natu
47             Lately rediscovered orthorhombic black phosphorus (BP) exhibits promising properties for
48 ly, photodetectors using van der Waals (vdW) black phosphorus (BP) flakes have demonstrated highly se
49 sotropic thermal-conductivity tensor of bulk black phosphorus (BP) for 80 </=T </= 300 K is reported.
50                                              Black phosphorus (BP) has been gathering great attention
51                                  Among them, black phosphorus (BP) is a 2D nanomaterial consisting of
52                                              Black phosphorus (BP) is a monoelemental 2D material pre
53                                              Black phosphorus (BP) is a narrow bandgap layered semico
54                                    Few-layer black phosphorus (BP) is a new two-dimensional material
55                                              Black phosphorus (bP) is a two-dimensional van der Waals
56 e induced by oxidation-related defects in 2D black phosphorus (BP) is exploited to achieve visual mem
57 aphene (PG) surface plasmons and anisotropic black phosphorus (BP) localized surface plasmons, which
58                                           2D black phosphorus (BP) nanomaterials are presented as a d
59 photoelectric, and photocatalytic effects of black phosphorus (BP) nanosheets, a BP-PAO fiber with en
60                                              Black phosphorus (BP) offers considerable promise for in
61  an ultra-low contact resistance few-layered black phosphorus (BP) transistor with metallic PGex cont
62      The limited stability of the surface of black phosphorus (BP) under atmospheric conditions is a
63                                              Black phosphorus (BP) with unique 2D structure enables t
64 ub-mean free path (MFP) scaled vertical InSe/black phosphorus (BP)(5-9) heterostructures(10).
65 isotropic thermal conductivity of passivated black phosphorus (BP), a reactive two-dimensional materi
66                                    Few-layer black phosphorus (BP), also known as phosphorene, is poi
67                                              Black phosphorus (BP), an emerging layered material, has
68 m nitride (hBN) with a few layer phosphorene black phosphorus (BP), hBN/BP/hBN heterostructures are m
69     Fibrous Phosphorus (FP), an allotrope of black phosphorus (BP), is one of the most promising cand
70 ion metal dichalcogenides (e.g., MoS2, WS2), black phosphorus (BP), metal nanosheets and two-dimensio
71  interaction and ease of oxidation issues of black phosphorus (BP), the domain size of artificial syn
72                          Here we reintroduce black phosphorus (BP), the most stable allotrope of phos
73 emission spectral distributions of monolayer black phosphorus (BP), which are governed by the symmetr
74                                              Black phosphorus (BP), with a mid-infrared (MIR) bandgap
75                                   Exfoliated black phosphorus (BP)-a layered two-dimensional semicond
76                                              Black phosphorus (bP)-based MWIR light emitters and dete
77 n and passivation of mechanically exfoliated black phosphorus (BP).
78 on (SSPM) effect for solution dispersions of black phosphorus (BP).
79 -based PTAs such as graphene, Au, MoS2 , and black phosphorus (BP).
80 , an injectable dual-network hyaluronic acid/black phosphorus (BP)/ fibroblast growth factor 21 (FGF2
81 plane anisotropy of a flexible thin flake of black-phosphorus (BP), we devise plasma-wave, thermoelec
82            We report that few-layer pristine black phosphorus channels passivated in an inert gas env
83                                              Black phosphorus consists of stacked layers of phosphore
84 dual PNRs by ionic scissoring of macroscopic black phosphorus crystals.
85 fabricated by ultrasonication of macroscopic black phosphorus crystals.
86                    Our results shed light on black phosphorus degradation which can aid future passiv
87 y barrier heights for electrons and holes in black phosphorus devices for a large range of body thick
88 ), while the previously known alpha form and black phosphorus display the more common chair conformat
89 on of a widely tunable band gap in few-layer black phosphorus doped with potassium using an in situ s
90                               Each few-layer black phosphorus exhibits a thickness-dependent unique i
91          Phosphorene, monolayer or few-layer black phosphorus, exhibits fascinating anisotropic prope
92 ering in dual gated molybdenum disulfide and black phosphorus FETs.
93 d materials, namely molybdenum disulfide and black phosphorus field effect transistors (FETs), as a c
94 PPs, at THz frequencies, in hBN-encapsulated black phosphorus field effect transistors through THz ne
95                                          The black phosphorus film hosting the 2DEG is placed on a he
96 tio is found to be approximately 2 for thick black phosphorus films and drops to approximately 1.5 fo
97                    Surface scattering in the black phosphorus films is shown to strongly suppress the
98 ly 20 and approximately 40 W m(-1) K(-1) for black phosphorus films thicker than 15 nm, respectively,
99 ain size of artificial synthesized few-layer black phosphorus (FL-BP) crystals is often below 10 um,
100                                  Research on black phosphorus has been experiencing a renaissance ove
101                                              Black phosphorus has been revisited recently as a new tw
102                                      Layered black phosphorus has drawn much attention due to the exi
103                                      Lately, black phosphorus has emerged as a promising new two-dime
104                                              Black phosphorus has emerged as a unique optoelectronic
105 lack phosphorene (BP, monolayer or few-layer black phosphorus) has gained much attention in various f
106        Phosphorene, a single atomic layer of black phosphorus, has recently emerged as a new two-dime
107  approach starting from a few layers of bulk black phosphorus, have failed to produce reliably precis
108 t-assisted exfoliation and postprocessing of black phosphorus in deoxygenated water.
109   No superconductivity could be achieved for black phosphorus in its normal orthorhombic form, despit
110 D semiconductors including MoS(2), InSe, and black phosphorus in monolayer form, and is the highest a
111               The use of anisotropic layered black phosphorus in polarization-sensitive photodetectio
112       Here, the authors demonstrate a stable black phosphorus ink suitable for printed ultrafast lase
113                               Here we show a black phosphorus ink that can be reliably inkjet printed
114 ctrochemical unzipping of single crystalline black phosphorus into zigzag-phosphorene nanobelts, as w
115                        Recently rediscovered black phosphorus is a layered semiconductor with promisi
116                                              Black phosphorus is a two-dimensional material of great
117                                    Ultrathin black phosphorus is a two-dimensional semiconductor with
118                                              Black phosphorus is also known to be a superconductor un
119                                              Black phosphorus is an emerging layered material.
120                                              Black phosphorus is an infrared layered material.
121 anopatterning and layer-by-layer thinning of black phosphorus is demonstrated with conductive atomic-
122         Following encapsulation, the printed black phosphorus is stable against long-term (> 30 days)
123          However, environmental stability of black phosphorus is still a major issue, which hinders t
124 he surface carrier recombination velocity of black phosphorus is two orders of magnitude lower than t
125 ic TBR across a prototype 2D material, i.e., black phosphorus, is reported through a crystal-orientat
126 ional semiconductors such as atomically thin black phosphorus, is significantly affected by the elect
127         The practical application of layered black phosphorus (LBP) is compromised by fast decomposit
128  opposite potentials on the opposite ends of black phosphorus macroparticles thereby leading to its d
129 ydrogen evolution reaction (HER) relative to black phosphorus macroparticles.
130  values fall between those of alpha-GeSe and black phosphorus, making beta-GeSe a promising candidate
131                The tunable band structure of black phosphorus may allow great flexibility in design a
132  thermal conductivity of suspended few-layer black phosphorus measured by micro-Raman spectroscopy.
133 rated SKMs with electrically tunable bipolar black phosphorus-molybdenum disulfide (bP-MoS(2)) photod
134 representative 2D materials (e.g., graphene, black phosphorus, MoS(2), h-BN, WS(2), MoSe(2), and WSe(
135         A bifunctional separator modified by black-phosphorus nanoflakes is prepared to overcome the
136           The remarkable progress of applied black phosphorus nanomaterials (BPNMs) is attributed to
137                            Here we fabricate black phosphorus nanoparticles (BP NPs) by solution base
138                                   We utilize black phosphorus nanoparticles as electrocatalytic tags
139 plane thermal conductivity of single-crystal black phosphorus nanoribbons along the zigzag and armcha
140 on nickel-iron layered double hydroxide with black phosphorus nanosheets (AuNP/Ni-Fe LDH/BPNSs) compo
141         Here we demonstrate the potential of black phosphorus nanosheets (BPNSs) as a therapeutic age
142                                              Black phosphorus nanosheets (BPs) show great potential f
143 r the surface functionalization of few-layer black phosphorus nanosheets using a family of photolytic
144 c basal-plane thermal conductivities of thin black phosphorus obtained from a new four-probe measurem
145 le, we trace back to the research history on black phosphorus of over 100 years from the synthesis to
146 pectroscopy reveals dark exciton dynamics of black phosphorus on ~100 fs time scale and its anisotrop
147 sm in a transistor channel made of flakes of black-phosphorus or InAs nanowires.
148 nsor based on porous graphene functionalized black phosphorus (PG-BP) composite to detect of leptin.
149                                            A black phosphorus photodetector is utilized to investigat
150  the operational wavelength range of tunable black phosphorus photonic devices, but also pave the way
151      Our results, coupled with the fact that black phosphorus possesses anisotropic energy bands with
152               Here, we prepared a biomimetic black phosphorus quantum dot (BPQDs) formulation to indu
153 platform for printed devices.Atomically thin black phosphorus shows promise for optoelectronics and p
154                                    The first black-phosphorus synaptic device is demonstrated, which
155 er Waals materials- molybdenum disulfide and black phosphorus, their electrically tunable photorespon
156 e been developed for scalable exfoliation of black phosphorus, these techniques have thus far used an
157 r measurements indicate that PMMA passivated black phosphorus thin film flakes can stay pristine for
158  the free-carrier to excitonic transition in black phosphorus thin films, and differs from the behavi
159                                 In addition, black phosphorus, though rarely mentioned, is a layered
160  der Waals layered materials using tri-layer black phosphorus (TLBP) integrated in a Fabry-Perot cavi
161 terial properties, and extend the topic from black phosphorus to phosphorene.
162 te a broadband photodetector using a layered black phosphorus transistor that is polarization-sensiti
163 .365 kOmegamum, which is the lowest value in black phosphorus transistors without degradation of ION/
164      Here, we spatially Raman map exfoliated black phosphorus using confocal fast-scanning technique
165 pic and strongly bound excitons in monolayer black phosphorus using polarization-resolved photolumine
166        Furthermore, leveraging a 10 nm-thick black phosphorus, we continuously tune its bandgap from
167 ize a parity-forbidden dark exciton state in black phosphorus while maintaining its intrinsic materia
168 escence quantum yield at room temperature in black phosphorus while measuring the various radiative a
169 d study of mechanically exfoliated few-layer black phosphorus, with thickness ranging from 2 to 15 la

 
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