# | Title | Journal | Year | Citations |
---|
1 | Ultrahigh electron mobility in suspended graphene | Solid State Communications | 2008 | 6,963 |
2 | Raman spectroscopy of graphene and graphite: Disorder, electron–phonon coupling, doping and nonadiabatic effects | Solid State Communications | 2007 | 6,322 |
3 | The one phonon Raman spectrum in microcrystalline silicon | Solid State Communications | 1981 | 2,208 |
4 | The effects of microcrystal size and shape on the one phonon Raman spectra of crystalline semiconductors | Solid State Communications | 1986 | 2,057 |
5 | High ionic conductivity in lithium lanthanum titanate | Solid State Communications | 1993 | 1,348 |
6 | The electronic structure of h.c.p. Ytterbium | Solid State Communications | 1971 | 1,217 |
7 | The resonating valence bond state and high-Tc superconductivity — A mean field theory | Solid State Communications | 1987 | 1,165 |
8 | Substitutional doping of amorphous silicon | Solid State Communications | 1975 | 1,115 |
9 | Spin polarization of conduction electrons induced by electric current in two-dimensional asymmetric electron systems | Solid State Communications | 1990 | 1,114 |
10 | High-temperature superconductivity in the BaPb1-xBixO3 systems | Solid State Communications | 1975 | 1,112 |
11 | Quantum size effect in semiconductor microcrystals | Solid State Communications | 1985 | 1,096 |
12 | Giant dielectric constant response in a copper-titanate | Solid State Communications | 2000 | 1,031 |
13 | Superconducting fluctuations and the peierls instability in an organic solid | Solid State Communications | 1973 | 1,018 |
14 | Conductivity from charge or spin density waves | Solid State Communications | 1974 | 986 |
15 | Universal relationship of the resistivity and specific heat in heavy-Fermion compounds | Solid State Communications | 1986 | 978 |
16 | Charge transfer excitations and superconductivity in “ionic” metals | Solid State Communications | 1987 | 917 |
17 | Ultraviolet spontaneous and stimulated emissions from ZnO microcrystallite thin films at room temperature | Solid State Communications | 1997 | 916 |
18 | An alternative way of linearizing the augmented plane-wave method | Solid State Communications | 2000 | 897 |
19 | An analogy between superconductors and smectics A | Solid State Communications | 1972 | 895 |
20 | The superconductivity at 18 K in LiFeAs system | Solid State Communications | 2008 | 884 |
21 | Dielectric hysteresis in single crystal BiFeO3 | Solid State Communications | 1970 | 881 |
22 | Photonic crystals | Solid State Communications | 1997 | 868 |
23 | Relation of magneto-optical properties of free excitons to spin alignment of Mn2+ ions in Cd1−xMnxTe | Solid State Communications | 1979 | 857 |
24 | Epitaxial graphene | Solid State Communications | 2007 | 857 |
25 | One-dimensional nanostructures: Chemistry, physics & applications | Solid State Communications | 1998 | 855 |
26 | Comparative study on the excitons in lead-halide-based perovskite-type crystals CH3NH3PbBr3 CH3NH3PbI3 | Solid State Communications | 2003 | 850 |
27 | The origin of visible luminescencefrom “porous silicon”: A new interpretation | Solid State Communications | 1992 | 844 |
28 | The exchange-correlation energy of a metallic surface | Solid State Communications | 1975 | 791 |
29 | Electrical properties of bulk ZnO | Solid State Communications | 1998 | 781 |
30 | Band structure of elastic waves in two dimensional systems | Solid State Communications | 1993 | 758 |
31 | Photonic band gaps in three dimensions: New layer-by-layer periodic structures | Solid State Communications | 1994 | 721 |
32 | A physical interpretation of dispersive transport in disordered semiconductors | Solid State Communications | 1981 | 712 |
33 | Thermal properties of graphene and multilayer graphene: Applications in thermal interface materials | Solid State Communications | 2012 | 689 |
34 | Collective motions of hydrogen bonds | Solid State Communications | 1963 | 672 |
35 | Bonding in hydrogenated hard carbon studied by optical spectroscopy | Solid State Communications | 1983 | 669 |
36 | Room temperature spin polarized injection in organic semiconductor | Solid State Communications | 2002 | 663 |
37 | Microwave oscillations of current in III–V semiconductors | Solid State Communications | 1963 | 657 |
38 | Constraint theory, vector percolation and glass formation | Solid State Communications | 1985 | 654 |
39 | Glassy polarization behavior in ferroelectric compounds and | Solid State Communications | 1983 | 653 |
40 | On the photoionization of deep impurity centers in semiconductors | Solid State Communications | 1965 | 648 |
41 | Photoluminescence in TiO2 anatase single crystals | Solid State Communications | 1993 | 637 |
42 | Strong vortex pinning intrinsic in high-Tc oxide superconductors | Solid State Communications | 1989 | 636 |
43 | Observation of Raman band shifting with excitation wavelength for carbons and graphites | Solid State Communications | 1981 | 631 |
44 | The properties of five highly conducting salts: (TMTSF)2X, X = PF6-, AsF6-, SbF6-, BF4- and NO3-, derived from tetramethyltetraselenafulvalene (TMTSF) | Solid State Communications | 1980 | 618 |
45 | Crystal structure refinement of AlN and GaN | Solid State Communications | 1977 | 609 |
46 | Chemical effects on the frequencies of Si-H vibrations in amorphous solids | Solid State Communications | 1979 | 606 |
47 | Effect of static uniaxial stress on the Raman spectrum of silicon | Solid State Communications | 1970 | 603 |
48 | Optical spectroscopy of graphene: From the far infrared to the ultraviolet | Solid State Communications | 2012 | 601 |
49 | The chain structure of BaTiO3 and KNbO3 | Solid State Communications | 1968 | 598 |
50 | The atomic structure of BiFeO3 | Solid State Communications | 1969 | 583 |