Temperature studies of Fe−Mn nodules

Sea nodules were extensively studied over a wide range of temperature ranging from 77K to 1175K using Mossbauer effect and ESR. The Mossbauer studies of the nodules at 77K and room temperature show a quadrupole doublet whereas at higher temperatures magnetic spectra were obtained starting at around 875K which ultimately gives a hyperfine field of around 390 KOe at 1175 K. The Mossbauer spectra recorded at 30K did not show any significant change in the room temperature spectra. The analysis of the spectra upto 775K showed two positions of Fe^R+, vie., octahedral and tetrahedral which were varified by ESR of the diluted samples.     

Collisional narrowing and spectral shift in coherent anti-stokes Raman spectra of molecular nitrogen up to 2500 bar and 700 K

CARS spectra of the N₂ Q-branch up to 2500 bar and 700 K have been measured. Calculated spectra based on theoretical models show significant disagreement with measured spectra above 300 bar so that CARS temperature measurements are in error by 130 K at 700 K and –150 K at 295 K. The spectral shift of the Q-branch reaches an asymptotic value corresponding to that measured in liquid nitrogen.     

蒽分子晶体的喇曼散射

在室温和液氮温度下,用氩离子激光器的5145Å激光激发,测量了蒽单品的喇曼散射谱,其喇曼活性主模振动的实验值和理论值符合的较好。计算了旋转振动的均方振幅,并对低波数振动喇曼谱的温度效应进行了讨论。     

Valence transition of YbInCu4 observed in hard X-ray photoemission spectra

Yb 3d and valence-band photoemission spectra of the first-order valence-transition compound YbInCu4 have been measured with hard x ray at an excitation energy of 5.95 keV. Abrupt changes are clearly observed in both spectra around the transition temperature T(V)=42 K, in comparison with ultraviolet and soft x-ray photoemission (VUV-PES and SX-PES) spectra. From the Yb 3d spectra, the Yb valence has been estimated to be approximately 2.90 from 220 down to 50 K and approximately 2.74 at 30-10 K. We propose that Yb 3d hard x-ray photoemission spectroscopy is a very powerful method to estimate the valence of Yb with high accuracy. On the other hand, the Yb2+ 4f-derived peaks in the valence-band spectra exhibit a remarkable enhancement below T(V). The shape of the valence-band spectra is different from those of the VUV-PES and SX-PES spectra above T(V), reflecting the In 5s and 5p contributions.     

Study of the parameters of the He(3 <Superscript>3</Superscript>S)-He(2 <Superscript>3</Superscript>P) line *

We have observed emission spectrum in dense plasmas of helium excited by a corona discharge at 706.69 nm. In continuation of an analysis of spectra obtained in gaseous helium at 300 K, we report on a study of the line parameters of the observed spectra. We discuss the major importance of temperature and perturber density in the broadening, shift and asymmetry measured from calculated profiles within a unified line shape semi-classical theory. The comparison is done with existing data derived from experimental spectra at 300 K. The theoretical work is extended at lower temperatures down to 40 K.     

B and C band excitation and emission spectra in KI:T1

Abstract

We present the excitation spectra of KI:T1 measured in the region of the B and C absorption bands at several emission wavelengths and at 20 K, 80 K and 300 K. An accurate analysis of these spectra shows new properties of the excitation spectra, that we relate to the non radiative relaxation of the excited electrons towards the luminescent states.     

Iron distribution in chevkinite

In this paper Mössbauer spectra of chevkinite at 283K and 83K are presented for the first time. The spectra consist of two Fe²⁺ and two Fe³⁺ doublets, and the assignments were made according to the structure of chevkinite. Iron distribution obtained from the spectrum at 83 K is consistent with that at 283 K.     

Mössbauer relaxation spectra of LiNbO3: Fe(III)

Mössbauer spectra of LiNbO₃: Fe(III)-monocrystals were measured in zero external magnetic field (5mK to 673K). They all show typical lineshapes due to relaxation effects. Below 77K temperature independent and above 77K a temperature-dependent relaxation is observable. In spectra measured in external magnetic fields relaxation effects occur only above 77K. We present least square fits of spectra measured at 300K and external magnetic fields using symmetry invariant reservoir spectral densities. The applied numerical formalism takes the complete electronuclear manifold of⁵⁷Fe(III) into account. We discuss the problems concerning the interpretation of zero field spectra.     

光系统Ⅱ核心天线的低温荧光光谱及动力学研究

采用稳态及飞秒荧光光谱技术研究了光系统Ⅱ中核心复合物在83 K、160 K和273 K低温下的能量传递途径.激发波长为507 nm.随着温度的升高,稳态荧光光谱逐渐发生蓝移.通过对不同温度下稳态光谱进行高斯解析,获得5个特征叶绿素a分子, 分别为Chl a670.4670, Chl a681.9680, Chl a683.9683, Chl a687.5,687.8,689687和Chl a698.0690,其中仅有Chl a687.5,687.8,689687在3个温度下的光谱中都解析获得,并且其谱宽以及荧光比例都随着温度升高而增加,因此推断温度对CP47中易裂解的叶绿素a分子有较大的影响.在680 nm以及690 nm波长处对不同温度下的时间曲线利用F900时间处理系统进行拟合,获得73 ps、 110 ps、 186 ps、 246~972 ps和1~3.7 ns 5个时间组分.其中, 73 ps是电荷分离的时间;110 ps和186 ps是β-Car分子受激发后,将激发能最终传递给反应中心所需要的时间;246~972 ps是电荷重组的时间过程;而1~3.7 ns是激发态分子发生电荷重组后又衰退回到基态的时间.73 ps的时间组分只在83 K温度下得到,因此,随着温度降低,可以探测到快的时间组分. 此外,对光谱随温度升高而发生蓝移进行了分析.     

Low temperature laser absorption spectra of methane in the near-infrared at 1.65 μm for lower state energy determination

Direct absorption spectra of the 2v₃ band of methane (CH₄) from 6038 to 6050 cm^-1 were studied at different low temperatures using a newly developed cryogenic cell in combination with a distributed feedback (DFB) diode laser. The cryogenic cell can operate at any stabilized temperature ranging from room temperature down to 100 K with temperature fluctuation less than ±1 K within 1 hour. In the present work, the CH₄ spectra in the range of 6038-6050 cm^-1 were recorded at 296, 266, 248, 223, 198, and 176 K. The lower state energy E″ and the rotational assignment of the angular momentum J were determined by a “2-low-temperature spectra method” using the spectra recorded at 198 and 176 K. The results were compared with the data from the GOSAT and the recently reported results from Campargue and co-workers using two spectra measured at room temperature and 81 K. We demonstrated that the use of a 2-low-temperature spectra method permits one to complete the E″ and J values missed in the previous studies.     

Correlated ejection of electron-hole drops from a continuously generated electron-hole liquid in Ge

The photocurrent power spectra were measured in a Ge photodiode as a function of the incident optical intensity at 1.8 K and 4.3 K. The observed spectra showed a peak at low frequencies superimposed on a continuum which has a cut-off at high frequency. The interpretation of the results implies that the electron-hole drops coming from a same region of the photoexcited liquid are ejected periodically.     

Temperature dependence of phonon energy spectra with nuclear resonant scattering of synchrotron radiation

Summary The phonon energy spectra of a polycrystalline α-Fe foil were observed at 150 K and 300 K by using the nuclear resonant scattering of synchrotron radiation. In each spectrum, inelastic scattering was observed at both sides of the elastic peak. It was found that the ratio of the elastic-scattering component and the asymmetry of the intensity of the side bands observed at 150 K are larger than those observed at 300 K, respectively. The observed temperature-dependent spectra are in good agreement with the spectra calculated from the phonon energy distribution function. One of the advantageous features of this method is that the excitation of only a specific element is possible. Our results show that this method is applicable to the study of lattice dynamics and opens a new field of the nuclear resonant scattering spectroscopy. Paper presented at ICAME-95, Rimini, 10–16 September 1995.     

丙氨酸对映体单晶的变温偏振激光拉曼光谱研究

本文测量了在不同偏振状态下 ,D 和L 丙氨酸的变温拉曼光谱。我们发现 :1 丙氨酸对映体的非偏振拉曼光谱图极其相似。 2 着重研究了D 丙氨酸偏振拉曼光谱随温度变化的特点。 3 通过拉曼光谱的手段 ,我们未发现A Salam所预言的在 2 5 0K左右从D 丙氨酸→丙氨酸的二级相变。     

The role played by hydrogen in the ionic thermocurrents of beryl

Abstract

Ionic thermocurrents (ITC) were measured in pink (morganite) and colourless (goshenite) samples of natural beryl from 77K up to 250K at a constant rate b = 0.1 Ks^?1. The spectra present three distinct bands, at 170K, 200K and 220K. The band at 200K predominates in the untreated crystals. After thermal treatments between 700K and 1300K, the ITC bands at 170K and 220K become prominent, masking the 200K band. The reduction of Fe³⁺ into Fe²⁺ in two distinct positions in the beryl lattice justify this observation. Infrared (IR) spectra show that treatments above 1000K remove water from the channels of the beryls. Ultraviolet (UV) irradiation of these thermally treated samples enhance the two bands at 170K and 220K.     

I.R. reflection and transmission properties of KH2PO4

The i.r. a-axis reflection spectrum of KDP at 125K has been examined in the range 360-60 cm^?1, and the a — and c-axis reflection spectra have been measured at 290K in the range 700-10 cm^?1. The real and imaginary parts of the dielectric constants (?′ and ?″) have been obtained from the reflectivity measurements by Kramers-Kronig analyses. The low-frequency values of ?′ at 290K agree well with microwave values. The transmission spectra of thin KDP films at 290,125 and 110K have been examined and are found to be closely correlated with the ?″ spectra. We conclude that the films behave as if they contain crystallites of large surface area. A tentative identification of the lowest-frequency c-axis polar mode has been made in the 125K transmission spectrum.     

Electron delocaliztion in ilvaite

Mössbauer spectra of ilvaite at 473 K, 573K and 673 K were measured in this paper Mixed-valence states of iron on A sites of ilvaite was observed, and thermally electron delocalization was used to explain all spectra.     

新型酞菁的光致发光性质研究

研究了2,3-四-(2-异丙基一5-甲基苯氧基)氢酞菁在10,77,177和300 K下石英衬底上的浇铸膜和单晶硅衬底上真空镀膜(约200 nm厚)在300 K下光致发光光谱.氢酞菁的浇铸膜光致发光光谱在上述温度下均出现荧光发射和磷光发射峰,在177和300 K下出现了1 673 nm激基缔合物峰.该峰的出现与分子抗聚集能力的强弱有关,在300 K激基缔合物峰比在177 K下的峰强,从氢酞菁分子结构特点讨论了形成激基缔合物的原因.随着温度的升高,可以观察到荧光发射峰渐渐减弱而激基缔合物峰变强.由于浇铸膜和真空镀膜的酞菁分子聚集态不同导致了斯托克司位移的差异,真空镀膜的发光峰峰值在1 140 nm左右,与酞菁浇铸膜的峰值差别较大.浇铸膜的发光峰的半高宽为300 nm,而真空镀膜发光峰的半高宽为100 nm左右.     

Luminescence spectra of doped and undoped lead tungstate crystals

TL spectra of undoped lead tungstate crystals exhibit glow peaks at 30 v K and 85 v K centred at 440 v nm, plus a peak at 50 v K at 530 v nm in an annealed sample. Annealing adds a 170 v K peak. Trivalent dopants of La 3+ and Y 3+ reduce the green luminescence, and Nb 5+ introduces a peak near 100 v K centred at 530 v nm; Sb introduces features between 40 v K and 90 v K and 150 and 180 v K. The luminescence emissions around 50 v K may be attributed to complex intrinsic defect centres, including (WO 4 ) m 3 . Of the four dopants studied in the present research, Sb +5 has the highest luminescence intensity. CL spectra show interesting anomalies near 170 v K which are linked to a phase change of water/ice nanoparticles trapped at dislocations.     

Photoluminescence and photoconductivity of indium selenide single crystals doped with rare-earth elements

The paper discusses the results of the investigation of photolominescence spectra and photoconductivity spectral distribution of Nd-; Yb- and Er- doped InSe single crystals at 77 and 293 K. Rare-earth additions into InSe contributes to the appearance of new bands in the wavelength region 1.02÷1.06 mkm. The photoconductivity spectra obtained for the mentioned crystals at 77 and 293 K are given.     

Investigation of polarized low-frequency spectra of solid solutions of paradibromobenzene with parachloronitrobenzene in the β phase at 293 and 77 K

The polarized spectra of Raman scattering by lattice vibrations in solid solutions of paradibromobenzene with parachloronitrobenzene in the β phase are studied at temperatures of 297 and 77 K. It is found that the spectrum of the β phase at room temperature differs from the spectra of the α and γ phases, which agrees with the X-ray diffraction data. The crystals have a rodlike structure in the region of parachloronitrobenzene concentrations of 25–50% and 70–85% and do not have this structure at concentrations of 50–70% at room temperature. The analysis of the spectra at 77 K shows that the structure of the β phase consists of regions with the β phase structure and regions with the paradibromobenzene structure. The frequency spectra of the mixed crystal are calculated by the Dean method.