N. Ong - Academia.edu (original) (raw)
Papers by N. Ong
Physical Review B, 1998
ABSTRACT The resistivities and magnetic susceptibilities of the Ba3MRu2O9 series of compounds, wi... more ABSTRACT The resistivities and magnetic susceptibilities of the Ba3MRu2O9 series of compounds, with M=Fe, Co, Ni, Cu, and In, are reported. All compounds have regular or distorted versions of the hexagonal barium titanate structure, consisting of chains of face-sharing RuO6 octahedra interconnected by corner-sharing MO6 octahedra. The compounds are semiconductors with ρ>0.1 Ω cm at ambient temperature. The magnetic susceptibilities below 400 K show that the 3d elements display local moments, and that the variants with M=Co, Ni, and Cu have magnetic transitions near 100 K.
Physical review. B, Condensed matter, 1988
... University of Pennsylvania, Philadelphia, Pennsylvania 19104 RV Chamberlin Department of Phys... more ... University of Pennsylvania, Philadelphia, Pennsylvania 19104 RV Chamberlin Department of Physics, Arizona State University, Tempe, Arizona 85287 ZZ Wang, TW ... characterized by x-ray and other spectroscopies.8 The resistive transition (0.5 mA at 28 Hz) in zero field was at ...
Physical review. B, Condensed matter, 1987
The Hall coefficient R H , the volume fraction f showing the Meissner effect, and the superconduc... more The Hall coefficient R H , the volume fraction f showing the Meissner effect, and the superconducting transition temperature T c have been measured in the high-T c oxide YBa 2 Cu 3 O 7-y for a range of oxygen vacancy concentration 0.0<y<0.7. We find that R H , f, and T c are insensitive to ...
Physical Review B, 1991
ABSTRACT Measurements of the Hall coefficient RH and resistivity ρa of YBa2Cu3O7 disclose anomali... more ABSTRACT Measurements of the Hall coefficient RH and resistivity ρa of YBa2Cu3O7 disclose anomalies in their temperature (T) dependences. The 1/RH vs T curve has a negative curvature, while dρa/dT displays a previously unreported step near 290 K. The Hall conductivity σH follows an unusual 1/T3 dependence from 100 to 360 K. We contrast the results with predictions of conventional Bloch theory, and compare them with recent calculations based on large-U models. Implications for cyclotron damping at low T are discussed.
Physica B+C, 1985
... FISCHER D partement de la Mati re Condens e, Universit de Gen ve, 24 Quai Ernest-Ansermet, 12... more ... FISCHER D partement de la Mati re Condens e, Universit de Gen ve, 24 Quai Ernest-Ansermet, 1211 Gen ve-4, Switzerland XJ ZHANG* and NP ONG Department of Physics, University of Southern California, Los Angeles, CA 90089-0484, USA The compounds MMo6S8 (M ...
Physical Review B, 1988
The optical anisotropy of YBa2Cu3O7-x in the 0.08-5.6 eV region is investigated by polarized refl... more The optical anisotropy of YBa2Cu3O7-x in the 0.08-5.6 eV region is investigated by polarized reflectance measurements on single crystals, and by transmittance, reflectance, and ellipsometric measurements on oriented thin films. In the visible-near-uv spectral region the anisotropy is relatively mild, but a huge anisotropy is observed in the infrared. Here, the reflectance increases with decreasing frequency for both polraizations, consistent
Physical Review B, 1991
Infrared reflectivity of single-crystal BizM + tCo Oy (M =Ca,Sr,Ba; m = 1,2), Bi2Sr3Fe2O9 2, and ... more Infrared reflectivity of single-crystal BizM + tCo Oy (M =Ca,Sr,Ba; m = 1,2), Bi2Sr3Fe2O9 2, and BizSr2Mn06 z5, isomorphic to Bi-Cu-based high-T, oxides
Physical Review B, 1988
ABSTRACT
Physical Review B, 1989
As x increases in Bi4Sr3Ca3-xTmxCu4O16+y the Hall carrier density nH decreases linearly. The vari... more As x increases in Bi4Sr3Ca3-xTmxCu4O16+y the Hall carrier density nH decreases linearly. The variation is consistent with Mott-Hubbard behavior, but in conflict with band-structure results which ignore correlations. We find that the variation of Tc vs nH is nonmonotonic. The source of the large carrier population (0.4/Cu) in the undoped (x=0) compound is discussed.
Physical Review B, 1984
ABSTRACT
Physical Review B, 1994
The resistivity [rho] and Hall coefficient [ital R][sub [ital H]] have been measured for samples ... more The resistivity [rho] and Hall coefficient [ital R][sub [ital H]] have been measured for samples of the two-plane superconductor HgBa[sub 2]CaCu[sub 2]O[sub 6+[delta]] ([ital T][sub [ital c]][similar to]124 K) with different annealing histories. The observed temperature dependence [ital R][sub [ital H]][similar to]1/[ital T] (up to 470 K) matches the steep dependence previously seen in 90-K YBa[sub 2]Cu[sub 3]O[sub 7[minus][delta]] and
Physical Review B, 1989
ABSTRACT The in-plane resistivity Ï{sub {ital ab}} of 60-K YBaâCuâO{sub 7-{ital y}} is equal to ... more ABSTRACT The in-plane resistivity Ï{sub {ital ab}} of 60-K YBaâCuâO{sub 7-{ital y}} is equal to (340{plus minus}30) μΩ cm at 290 K and varies approximately linearly with temperature {ital T}. The anisotropy Ï{sub {ital c}}/Ï{sub ab} increases from {similar to}100 to 2000 as {ital T} decreases from 290 to 80 K. In the four crystals studied Ï{sub {ital c}} is observed to increase monotonically with decreasing {ital T}. This is an intrinsic property of the normal state which has not been explained by conventional transport theory.
Physical Review B, 1989
Single crystals of the n-type Nd-Ce-Cu-0 superconducting materials have been grown via a Aux tech... more Single crystals of the n-type Nd-Ce-Cu-0 superconducting materials have been grown via a Aux technique, and their structural and physical properties characterized. Optimum crystal growth conditions were arrived at from a survey of various compositions and temperatures. We determine that the charge composition (50 mol% Nd203-Ce02, 50 mol%%uo CuO) held at a temperature of 1300'C and followed by a slow cooling to 1000'C produces plateletlike crystals of the n-type phase Nd~Ce Cu04, which, after being annealed at 900'C in nitrogen, become superconducting. The limit of the Ce solubility is x =0. 18, and only crystals having a Ce content between 0.14 and 0.17 were found to superconductors, with the rnaximurn I', occurring at x =0.14. The oxygen uptake and loss in the Nd material is similar to that measured on La2Cu04 but occurs at higher temperatures (750'C instead of 500 C). The large Meissner fraction indicates bulk superconductivity. However, due to a complex microstructure or compositional (e.g. , oxygen) inhomogeneities in the crystal, zero resistance is dificult to achieve. The resistivity temperature dependence above T, is metalliclike, and linear above 150 K, in contrast to bulk ceramics. Finally, no evidence for rnagnetic ordering over the temperature range 4-350 K was observed for the superconducting Ce-doped Nd&CuO4 phase, whereas signs of magnetic ordering were found at 340 K for the undoped material. pounds (e.g. , insulating LazCuO4 doped with Sr leads to a 40 K superconducting La2 Sr CuO&, Refs. 6-8). The formation of Cu with a valence greater than 2 (i.e. , oxidation of Cu) implies the introduction of a hole charge state. These holes, or missing electrons, are the charge carriers in all these cuprate superconductors and they are called, for this reason, p type. Recently Tokura et al. discovered a new class of materials Nd2 Ce Cu04 which are n-type superconductors at 23 K. They did this by chemically reducing the Cu (i.e. , doping the system with electrons) in two steps: (1) the replacement of trivalent (Nd) by tetravalent ions (Ce), and (2) the removal of oxygen. This new superconducting phase still contains CuOz planes, but the carriers are electrons (n type) and not holes (p type). The n-type charcharacter has been determined by Hall and Seebeck measurements , ' and x-ray absorption measurements" on polycrystalline samples indicate the presence of Cu+ scaling with Ce. Additional evidence supporting n-type conductivity in these new electron-doped superconductors is that the replacement of oxygen by fluorine (i.e. , again a reduction of the Cu) also induces superconductivity. ' By replacing the Nd in the parent compound Nd2, Ce"Cu04by other rare earths (Pr, Sm, Eu), and the Ce by Th, additional new n-type superconducting phases have been synthesized. ' '
Physical Review B, 1988
The resistivity anisotropy has been measured in seven single crystals of YBa2Cu307. %e 6nd that t... more The resistivity anisotropy has been measured in seven single crystals of YBa2Cu307. %e 6nd that the anisotropy is between 56 and 110 at 290 K, increasing to -250 just above T, (90-93 K). While the out-of-plane resistivity p, is close to the Mott limit, the large in-plane ...
Physical Review B, 1988
We have studied the in-plane paraconductivity in single crystals of YBa2Cu3O7 with exceptionally ... more We have studied the in-plane paraconductivity in single crystals of YBa2Cu3O7 with exceptionally sharp transitions. For temperatures greater than ~1 K above the transition temperature Tc, we find good qualitative and some quantitative agreement with the two-dimmensional Aslamazov-Larkin theory. The jump to zero resistance occurs in a narrow interval of less than 0.5 K. Our data are inconsistent with the Lawrence-Doniach expression for crossover from two to three dimensions.
Physical Review B, 1985
Phase plots of ICDW (the charge-density-wave current) versus the applied electric field E are pre... more Phase plots of ICDW (the charge-density-wave current) versus the applied electric field E are presented for driving frequencies 300 kHz to 3 MHz in NbSe3. When E exceeds the threshold value, inductive behavior (I lags E) appears. The strong hysteresis observed is inconsistent with the single-oscillator model. We compare the results with predictions of the overdamped pendulum equation and the transient overshoot phenomenon.
Physical Review B, 1983
Phase-space plots of the ac charge-density-wave (CDW) current versus the ac voltage have been obt... more Phase-space plots of the ac charge-density-wave (CDW) current versus the ac voltage have been obtained in NbSe3 for frequencies 0.1-5 MHz. The strong inductive hysteresis observed is consistent with metastable states in the CDW and incompatible with classical oscillator models.
Physical Review B, 1998
ABSTRACT The resistivities and magnetic susceptibilities of the Ba3MRu2O9 series of compounds, wi... more ABSTRACT The resistivities and magnetic susceptibilities of the Ba3MRu2O9 series of compounds, with M=Fe, Co, Ni, Cu, and In, are reported. All compounds have regular or distorted versions of the hexagonal barium titanate structure, consisting of chains of face-sharing RuO6 octahedra interconnected by corner-sharing MO6 octahedra. The compounds are semiconductors with ρ>0.1 Ω cm at ambient temperature. The magnetic susceptibilities below 400 K show that the 3d elements display local moments, and that the variants with M=Co, Ni, and Cu have magnetic transitions near 100 K.
Physical review. B, Condensed matter, 1988
... University of Pennsylvania, Philadelphia, Pennsylvania 19104 RV Chamberlin Department of Phys... more ... University of Pennsylvania, Philadelphia, Pennsylvania 19104 RV Chamberlin Department of Physics, Arizona State University, Tempe, Arizona 85287 ZZ Wang, TW ... characterized by x-ray and other spectroscopies.8 The resistive transition (0.5 mA at 28 Hz) in zero field was at ...
Physical review. B, Condensed matter, 1987
The Hall coefficient R H , the volume fraction f showing the Meissner effect, and the superconduc... more The Hall coefficient R H , the volume fraction f showing the Meissner effect, and the superconducting transition temperature T c have been measured in the high-T c oxide YBa 2 Cu 3 O 7-y for a range of oxygen vacancy concentration 0.0<y<0.7. We find that R H , f, and T c are insensitive to ...
Physical Review B, 1991
ABSTRACT Measurements of the Hall coefficient RH and resistivity ρa of YBa2Cu3O7 disclose anomali... more ABSTRACT Measurements of the Hall coefficient RH and resistivity ρa of YBa2Cu3O7 disclose anomalies in their temperature (T) dependences. The 1/RH vs T curve has a negative curvature, while dρa/dT displays a previously unreported step near 290 K. The Hall conductivity σH follows an unusual 1/T3 dependence from 100 to 360 K. We contrast the results with predictions of conventional Bloch theory, and compare them with recent calculations based on large-U models. Implications for cyclotron damping at low T are discussed.
Physica B+C, 1985
... FISCHER D partement de la Mati re Condens e, Universit de Gen ve, 24 Quai Ernest-Ansermet, 12... more ... FISCHER D partement de la Mati re Condens e, Universit de Gen ve, 24 Quai Ernest-Ansermet, 1211 Gen ve-4, Switzerland XJ ZHANG* and NP ONG Department of Physics, University of Southern California, Los Angeles, CA 90089-0484, USA The compounds MMo6S8 (M ...
Physical Review B, 1988
The optical anisotropy of YBa2Cu3O7-x in the 0.08-5.6 eV region is investigated by polarized refl... more The optical anisotropy of YBa2Cu3O7-x in the 0.08-5.6 eV region is investigated by polarized reflectance measurements on single crystals, and by transmittance, reflectance, and ellipsometric measurements on oriented thin films. In the visible-near-uv spectral region the anisotropy is relatively mild, but a huge anisotropy is observed in the infrared. Here, the reflectance increases with decreasing frequency for both polraizations, consistent
Physical Review B, 1991
Infrared reflectivity of single-crystal BizM + tCo Oy (M =Ca,Sr,Ba; m = 1,2), Bi2Sr3Fe2O9 2, and ... more Infrared reflectivity of single-crystal BizM + tCo Oy (M =Ca,Sr,Ba; m = 1,2), Bi2Sr3Fe2O9 2, and BizSr2Mn06 z5, isomorphic to Bi-Cu-based high-T, oxides
Physical Review B, 1988
ABSTRACT
Physical Review B, 1989
As x increases in Bi4Sr3Ca3-xTmxCu4O16+y the Hall carrier density nH decreases linearly. The vari... more As x increases in Bi4Sr3Ca3-xTmxCu4O16+y the Hall carrier density nH decreases linearly. The variation is consistent with Mott-Hubbard behavior, but in conflict with band-structure results which ignore correlations. We find that the variation of Tc vs nH is nonmonotonic. The source of the large carrier population (0.4/Cu) in the undoped (x=0) compound is discussed.
Physical Review B, 1984
ABSTRACT
Physical Review B, 1994
The resistivity [rho] and Hall coefficient [ital R][sub [ital H]] have been measured for samples ... more The resistivity [rho] and Hall coefficient [ital R][sub [ital H]] have been measured for samples of the two-plane superconductor HgBa[sub 2]CaCu[sub 2]O[sub 6+[delta]] ([ital T][sub [ital c]][similar to]124 K) with different annealing histories. The observed temperature dependence [ital R][sub [ital H]][similar to]1/[ital T] (up to 470 K) matches the steep dependence previously seen in 90-K YBa[sub 2]Cu[sub 3]O[sub 7[minus][delta]] and
Physical Review B, 1989
ABSTRACT The in-plane resistivity Ï{sub {ital ab}} of 60-K YBaâCuâO{sub 7-{ital y}} is equal to ... more ABSTRACT The in-plane resistivity Ï{sub {ital ab}} of 60-K YBaâCuâO{sub 7-{ital y}} is equal to (340{plus minus}30) μΩ cm at 290 K and varies approximately linearly with temperature {ital T}. The anisotropy Ï{sub {ital c}}/Ï{sub ab} increases from {similar to}100 to 2000 as {ital T} decreases from 290 to 80 K. In the four crystals studied Ï{sub {ital c}} is observed to increase monotonically with decreasing {ital T}. This is an intrinsic property of the normal state which has not been explained by conventional transport theory.
Physical Review B, 1989
Single crystals of the n-type Nd-Ce-Cu-0 superconducting materials have been grown via a Aux tech... more Single crystals of the n-type Nd-Ce-Cu-0 superconducting materials have been grown via a Aux technique, and their structural and physical properties characterized. Optimum crystal growth conditions were arrived at from a survey of various compositions and temperatures. We determine that the charge composition (50 mol% Nd203-Ce02, 50 mol%%uo CuO) held at a temperature of 1300'C and followed by a slow cooling to 1000'C produces plateletlike crystals of the n-type phase Nd~Ce Cu04, which, after being annealed at 900'C in nitrogen, become superconducting. The limit of the Ce solubility is x =0. 18, and only crystals having a Ce content between 0.14 and 0.17 were found to superconductors, with the rnaximurn I', occurring at x =0.14. The oxygen uptake and loss in the Nd material is similar to that measured on La2Cu04 but occurs at higher temperatures (750'C instead of 500 C). The large Meissner fraction indicates bulk superconductivity. However, due to a complex microstructure or compositional (e.g. , oxygen) inhomogeneities in the crystal, zero resistance is dificult to achieve. The resistivity temperature dependence above T, is metalliclike, and linear above 150 K, in contrast to bulk ceramics. Finally, no evidence for rnagnetic ordering over the temperature range 4-350 K was observed for the superconducting Ce-doped Nd&CuO4 phase, whereas signs of magnetic ordering were found at 340 K for the undoped material. pounds (e.g. , insulating LazCuO4 doped with Sr leads to a 40 K superconducting La2 Sr CuO&, Refs. 6-8). The formation of Cu with a valence greater than 2 (i.e. , oxidation of Cu) implies the introduction of a hole charge state. These holes, or missing electrons, are the charge carriers in all these cuprate superconductors and they are called, for this reason, p type. Recently Tokura et al. discovered a new class of materials Nd2 Ce Cu04 which are n-type superconductors at 23 K. They did this by chemically reducing the Cu (i.e. , doping the system with electrons) in two steps: (1) the replacement of trivalent (Nd) by tetravalent ions (Ce), and (2) the removal of oxygen. This new superconducting phase still contains CuOz planes, but the carriers are electrons (n type) and not holes (p type). The n-type charcharacter has been determined by Hall and Seebeck measurements , ' and x-ray absorption measurements" on polycrystalline samples indicate the presence of Cu+ scaling with Ce. Additional evidence supporting n-type conductivity in these new electron-doped superconductors is that the replacement of oxygen by fluorine (i.e. , again a reduction of the Cu) also induces superconductivity. ' By replacing the Nd in the parent compound Nd2, Ce"Cu04by other rare earths (Pr, Sm, Eu), and the Ce by Th, additional new n-type superconducting phases have been synthesized. ' '
Physical Review B, 1988
The resistivity anisotropy has been measured in seven single crystals of YBa2Cu307. %e 6nd that t... more The resistivity anisotropy has been measured in seven single crystals of YBa2Cu307. %e 6nd that the anisotropy is between 56 and 110 at 290 K, increasing to -250 just above T, (90-93 K). While the out-of-plane resistivity p, is close to the Mott limit, the large in-plane ...
Physical Review B, 1988
We have studied the in-plane paraconductivity in single crystals of YBa2Cu3O7 with exceptionally ... more We have studied the in-plane paraconductivity in single crystals of YBa2Cu3O7 with exceptionally sharp transitions. For temperatures greater than ~1 K above the transition temperature Tc, we find good qualitative and some quantitative agreement with the two-dimmensional Aslamazov-Larkin theory. The jump to zero resistance occurs in a narrow interval of less than 0.5 K. Our data are inconsistent with the Lawrence-Doniach expression for crossover from two to three dimensions.
Physical Review B, 1985
Phase plots of ICDW (the charge-density-wave current) versus the applied electric field E are pre... more Phase plots of ICDW (the charge-density-wave current) versus the applied electric field E are presented for driving frequencies 300 kHz to 3 MHz in NbSe3. When E exceeds the threshold value, inductive behavior (I lags E) appears. The strong hysteresis observed is inconsistent with the single-oscillator model. We compare the results with predictions of the overdamped pendulum equation and the transient overshoot phenomenon.
Physical Review B, 1983
Phase-space plots of the ac charge-density-wave (CDW) current versus the ac voltage have been obt... more Phase-space plots of the ac charge-density-wave (CDW) current versus the ac voltage have been obtained in NbSe3 for frequencies 0.1-5 MHz. The strong inductive hysteresis observed is consistent with metastable states in the CDW and incompatible with classical oscillator models.