Besides that, some authors had explored the potential association

Besides that, some authors had explored the potential association between the SULT1A1 polymorphism and breast cancer risk and it had also shown inconsistent results. Kotnis’ study showed that the polymorphism of SULT1A1 Arg213His might predispose carriers to lung cancers, protect against colorectal cancers and increase the risk of breast cancer to Asian women but not the Caucasian women [11]. Recently Wang et al. meta-analyzed the relationships between SULT1A1 and breast cancer risk [12] and concluded

that there was no significant relationship between SULT1A1 R213 H polymorphism and the risk of breast cancer. However both meta-analysis were not perfect and may lead to underestimate Adavosertib order the role of mTOR inhibitor SULT1A1 polymorphism in breast carcinogenesis, because they did not include some eligible studies and neglected the valuable subgroup analysis such as menopausal status. It should be pointed out that there was new finding in results of the present study which was never founded in the previous. The

current meta-analysis approved to be a more precise estimation which included two more studies and a subgroup analysis according to menses status which came out statistical significance. Here we performed an updated meta-analysis which was specialized in breast cancer, including 16 studies with a subgroup analysis based on ethnicity and menopausal status, using Arg/Arg vs His/His, Arg/Arg vs Arg/His, dominant model (Arg/His+His/His vs Arg/Arg) and recessive model (His/His vs Arg/Arg+Arg/His). Protein Tyrosine Kinase inhibitor Methods Identification and analysis of relevant studies Two investigators (Yiwei Jang and Liheng Zhou) independently obtained relevant articles through searches of PubMed, EBSCO and Web of Science databases using the following words: ‘sulfotransferase or SULT’, ‘polymorphism’ and ‘breast cancer’. Studies had been case-control design and based on SULT1A1 Arg213His polymorphism either alone

or in combination with other genes Staurosporine and the language of publication was restricted to English. All of the studies required study design, publication, breast cancer cases, controls selection and genotyping methods. We excluded articles on only breast cancer patients or on healthy persons and one case-series study. In the end, 10362 breast cancer patients and 14250 controls from 16 case-control studies were selected for this meta-analysis. Data extraction The following data were collected from each included studies: first authors, year of publications, study population (categorized as Asian, Caucasian, African and others), sources of controls, menopausal status and the number of different genotype in all subjects.

​doc Cited 29 Oct 2009 Taboada A, Kotze DJ, Tárrega R et al (200

​doc. Cited 29 Oct 2009 Taboada A, Kotze DJ, Tárrega R et al (2006) Traditional forest management: do carabid beetles respond to human-created vegetation structures in an oak mosaic landscape? Forest Ecol Manage 237:436–449CrossRef Terzi M, Marvulli M (2006) Priority zones for Mediterranean protected agro-sylvo-pastoral landscapes. Ecol Medit 32:29–38 Tucker GM, Evans MI (1997) Habitats for birds in Europe. A conservation strategy for the wider environment. BirdLife International, Cambridge Vera FW (2000) Grazing ecology and forest history. CABI, WallingfordCrossRef”
“Introduction

There is a deep-rooted tradition of studying spatial variation in species composition and delineating Captisol solubility dmso distinct ecological areas in terms of differences in species composition. At present, an understanding

of the spatial variation in biotic composition and its underlying mechanisms is pivotal to conservation biology (Margules and Pressey 2000). In recent decades, species richness has declined rapidly (Thomas et al. 2004; Millennium Ecosystem Assessment 2005), urging effective conservation and restoration strategies. Ensuing research has yielded numerous strategies for nature conservation. Efforts to prioritize areas for nature conservation worldwide have included circumscribing ‘hotspots’; areas with high species diversity or high levels of endemic, rare, or threatened species H 89 mouse (Myers et al. 2000; Margules et al. 2002; Fox and Beckley 2005; Tchouto et al. 2006). However, concentrations of overall species diversity Rebamipide and

of endangered and endemic species do not necessarily coincide (Prendergast et al. 1993; Orme et al. 2005). A refined method to select areas with high conservation value is to estimate an area’s complementarity: the context-dependent, marginal gain in biodiversity that its preservation would provide. Reserve selection methods based on the KPT-330 price complementarity principle and the use of advanced computer algorithms are popular (Rodrigues and Gaston 2002; Williams et al. 2006) but, according to Faith et al. (2003), nowhere have the sets of areas thus selected been implemented in regional conservation planning. In the absence of basic, fine-scaled data on the distribution of most species, both approaches depend on surrogate information. As distribution patterns do not necessarily coincide for different taxonomic groups, it is debatable whether indicator, umbrella, or keystone taxa could serve as surrogates for total biodiversity (Williams and Gaston 1994; Andelman and Fagan 2000; Ricketts et al. 2002; Kati et al. 2004; Wiens et al. 2008). It is also debatable whether the focus should be on mammals, birds, and vascular plants, the dominant trend in conservation research and policy, instead of on overall biodiversity, healthy ecosystems, or the Earth’s genetic library (Jepson and Canney 2001). A different approach is to use specific environmental conditions (Pienkowski et al.

CrossRef 15 Dewey F, Yohalem D: Detection, quantification and im

CrossRef 15. Dewey F, Yohalem D: Detection, quantification and immunolocalisation of Botrytis p38 MAPK inhibitor species. In Botrytis: Biology, Pathology and Control. Volume Chapter 11. Edited by: Elad Y, et al. London; 2007:181–194. 16. Eriksson R, Jobs M, Ekstrand C, Ullberg M, Herrmann B, Landegren U, Nilsson M, Blomberg J: Multiplex and quantifiable detection of nucleic acid from pathogenic fungi using padlock probes, generic real time PCR and specific suspension array readout. J Microbiol Meth 2009, 78:195–202.CrossRef www.selleckchem.com/products/KU-55933.html 17. Gao X, Jackson K, Lambert S, Hartman G, Niblack T: Detection and quantification

of Fusarium solani in soybean roots with real-time quantitative polymerase chain reaction. Plant Dis 2004, 88:1372–1380.CrossRef 18. Leisova L, Minarikova V, Kucera L, Ovesna J: Quantification of Pyrenophora teres in infected barley leaves using real-time PCR. J Microbiol Meth 2006, 67:446–455.CrossRef 19. Lopez M, Bertolini E, Olmos A, Caruso P, Gorris M, Llop P, Penyalver R, Cambra M: Innovative tools for detection of plant pathogenic viruses and bacteria. Int Microbiol 2003, 6:233–243.PubMedCrossRef

20. McCartney H, Foster S, Fraaije B, Ward E: Molecular diagnostics for fungal plant pathogens. Pest Manag Sci 2003, 59:129–142.PubMedCrossRef 21. Savazzini F, Oliveira Longa C, Pertot I, Gessler C: Real-time PCR for detection and quantification of the biocontrol agent Trichoderma atroviride strain SC1 in soil. J Microbiol Meth 2008, 73:185–194.CrossRef 22. Schaad N, Frederick R: Real-time PCR and Selleckchem A-1210477 its application for rapid plant disease diagnostics. Can J Plant Pathol 2002, 24:250–258.CrossRef 23. Ward E, Foster S, Fraaije click here B, McCartney H: Plant pathogen diagnostics: immunological and nucleic acid-based approaches. Ann Appli Biol 2004, 145:1–16.CrossRef 24. Xie Z, Thompson A, Kashleva H, Dongari-Bagtzoglou A: A quantitative real-time RT-PCR assay for mature C. albicans biofilms. BMC Microbiology 2011, 11:93–100.PubMedCrossRef 25. Serrano R, Gusmão L, Amorim

A, Araujo R: Rapid identification of Aspergillus fumigatus within the section Fumigati. BMC Microbiology 2011, 11:82–88.PubMedCrossRef 26. He F, Soejoedono RD, Murtini S, Goutama M, Kwang J: Complementary monoclonal antibody-based dot ELISA for universal detection of H5 avian influenza virus. BMC Microbiology 2010, 10:330–338.PubMedCrossRef 27. Rigano LA, Marano MR, Castagnaro AP, Do Amaral AM, Vojnov AA: Rapid and sensitive detection of Citrus Bacterial Canker by loop-mediated isothermal amplification combined with simple visual evaluation methods. BMC Microbiology 2010, 10:176–183.PubMedCrossRef 28. Dewey F, Ebeler S, Adams D, Noble A, Meyer U: Quantification of Botrytis in grape juice determined by a monoclonal antibody-based immunoassay. Am J Enol Vitic 2000, 51:276–282. 29. Meyer U, Spotts R, Dewey F: Detection and quantification of Botrytis cinerea by ELISA in pear stems during cold storage. Plant Dis 2000, 84:1099–1103.CrossRef 30.

1997) The ultrastructure of R capsulatus fnrL null mutant bacte

1997). The ultrastructure of R. capsulatus fnrL null mutant bacteria, strains RGK295 and 296 (Table 1), was evaluated by preparing thin sections of cells cultured under low-oxygen conditions and examining them using TEM (Fig. 4B). In contrast to the abnormal appearance of R. sphaeroides FnrL− mutant bacterial cell membranes (Fig. 4A), the membrane morphology of R. capsulatus FnrL− bacteria appeared similar to the FnrL+ parent strain SB1003 (Table 1). Therefore, for R. capsulatus, the absence of FnrL apparently did not affect ICM formation.

This predicts that there are genes necessary for ICM development in R. sphaeroides whose transcription is regulated by FnrL, but that in R. capsulatus are not FnrL-dependent (or absent). Discussion Transcriptomic and proteomic investigations have provided AMPK inhibitor insights into regulatory events that are mediated by PrrA, PpsR, and mTOR inhibitor FnrL as R. sphaeroides responds to changes in oxygen availability (reviewed in Gomelsky and Zeilstra-Ryalls 2013). Spectral analysis has also been a useful tool in studying the roles of these DNA binding proteins in the formation of pigment–protein complexes. This study of membrane structure in mutants missing one or more of these global regulators has provided a different perspective and has generated new findings. Based on the TEM results, the prr genes are required for normal ICM formation. An unanticipated and

novel discovery made during these studies was the ultrastructural differences of low-oxygen cells with defective prrA genes versus those in which the entire prr gene cluster is absent. The presence of ICM-like structures in prrA null mutant bacteria and their absence in prrBCA − bacteria suggests that PrrB and/or PrrC may participate in regulation of genes associated with ICM formation that does not involve PrrA activity. To what degree these ICM-like structures resemble true ICM will require an in-depth analysis of their molecular composition. While for cells cultured anaerobically in the dark transcriptomic and proteomic data are available,

which could be used as a guide to direct us to potentially important genes regulated by PrrA involved in ICM formation, there is currently no similar data available at the Coproporphyrinogen III oxidase genome wide level for PrrB or C, nor for cells grown under low-oxygen conditions. Before this investigation, the presence of such structures, and so the need for such information was not evident, since other methods used to evaluate the physiological status of R. sphaeroides, such as comparisons of growth rates or even spectral analyses, gave no indication that there were any differences between cells lacking prrA alone versus those lacking all three prr genes under any condition. It is possible that the ultrastructure differences might be selleckchem explained by cross-talk or branched regulation between PrrB and a non-cognate response regulatory protein.

Endoscopy also provides excellent visualization of the mucosa to

Endoscopy also provides excellent visualization of the mucosa to evaluate for subtle and gross changes in the rectal mucosa. Endoscopy can serve as a middle ground in many cases to avoid surgical exploration by enabling evaluation and therapeutic removal of objects that may have been nonamenable to transanal extraction. Once successful extraction has been accomplished, the endoscope should be passed again to evaluate the bowel mucosa for any inadvertent injuries.

If the local perianal block and sedation are unsuccessful in the emergency department, the patient needs to be brought to the operating room for a general or spinal anesthetic to aid in the removal of the object. After anesthesia has been applied and the patient is adequately

relaxed, if the foreign body cannot be removed from below then a #BMN-673 randurls[1|1|,|CHEM1|]# laparotomy is indicated [3, 4]. Surgery is also indicated in all patients who present with perforation (free air), sepsis, or peritonitis. Some surgeons have also described laparoscopy as an aid to push the object more distally into the rectum for a transanal removal. The first step is to attempt to milk the object distally into the rectum. If this fails, then a colotomy and removal of the foreign object is needed. This colotomy can be primarily repaired. Diversion is reserved for patients with frank peritonitis and instability, perforation with extensive fecal contamination [3, 4]. The Selleckchem LCZ696 most dangerous complication of a rectal foreign body is perforation. When patients present with a rectal perforation, they should at first be stabilized like any trauma patient. After stabilization, management depends on 3 factors: first, whether the patient is clinically stable or unstable, second, whether the perforation is in an intraperitoneal or extraperitoneal location, and last, whether there is significant fecal soilage or not. A good rule of thumb is to manage a rectal perforation from a foreign body are diversion, Sunitinib research buy debridement, distal washout, and drainage. Unstable patients, those with multiple comorbidities, and those with significant tissue damage and de-layed presentation more often require a

diversion. On the other hand, patients who present early after the insult, those with minimal tissue damage, and those with little to no contamination can be managed with primary repair and washout. Small extraperitoneal injuries can also be managed with observation, avoidance of oral feeding, and antibiotics. However laparoscopic approach has been successfully aplied in the treatment of colonic perforations, where equivalent operative outcomes as open procedures can be accomplished in selected patients [11]. Postremoval observation depends on several factors, such as the clinical status of the patient, comorbidities, delay in presentation, and whether or not there was any resultant trauma to the rectum or surrounding tissue. Postextraction endoscopy and plain radiographs are a must before discharging any patient who had a foreign body removal [3–5].

56 and 150 MHz and with different power application positions A

56 and 150 MHz and with different power application positions. A two-dimensional (1 m × 0.2 m) plane electrode was modeled, and the impedances of the atmospheric-pressure plasma obtained from IV (current and voltage) measurements and analysis [7] were used for the calculation. Methods Modeling A one-dimensional model of electrodes and plasma (including

sheath) is shown in Figure 1. Radio-frequency voltage is applied to the upper electrode, and the lower electrode is grounded. We assume that only the upper electrode has resistance and inductance for simplicity. This simplified model is useful enough to calculate a relative voltage between two electrodes, because only relative voltage is important for plasma. Figure 1 One-dimensional model of electrodes Liproxstatin-1 ic50 and plasma (including sheath). Plasma will be generated in the space between the upper and lower electrodes. In this model, electrodes (upper and lower) and plasma are divided into small elements of length ΔX. The voltage U is assumed to be constant within the elements. Symbol δ is the thickness of current flow (skin depth). The currents flowing into and out from the element Selleck PF-573228 are shown by the arrows in Figure 1. The plasma is assumed to be able to be represented by the parallel connection of the capacitance C p and the conductance G p. One can derive a one-dimensional

wave equation from the above mentioned one-dimensional model and extend it to the following two-dimensional wave equation. In the case of a two-dimensional model, the electrode will be divided in two directions, and the widths of the element will be ΔX and ΔY. For MK-0457 mw simplicity, the element widths ΔX and ΔY were set to be equal. (1) Here, L and R are inductance and resistance per unit length (in current flow direction) of the electrodes of element width (ΔX or ΔY), and C p and G p are www.selleck.co.jp/products/MDV3100.html the capacitance and conductance of plasma per unit length of element width, respectively. F(x,y,t) is the external force (causes voltage to change) applied to the upper electrode

at position (x,y). Electrode resistance R and inductance L When radio-frequency power is applied to the electrodes, the current will flow only on the surface of the electrodes owing to the skin effect. The effective electrode resistance per unit length R (of width w) is determined by the following equation [8]: (2) where σ is the conductivity of the electrode material, δ is the skin depth, and w is the width of the current flow. The skin depth δ is determined by (3) where ω is the angular frequency, and μ is the magnetic permeability of the electrode material. The inductance of a pair of two parallel plates (electrodes) per unit length (of width w) can be calculated using [8] (4) where d is the distance between the upper and lower electrodes, and w is the width of the current flow. When aluminum is used as the electrode material, the conductivity σ is 0.

It is interesting to note that the

It is interesting to note that the reflected wave reverses direction within 10 minutes, without first forming a detectable stationary subpopulation, contrary to previous observations where reflected waves reverse direction on much longer time scales (~1 h), after first forming a stationary population [38]. We observe similar collision patterns between colonization waves even when both sides of the habitat are inoculated with cells from the same strain, indicating that these collisions are not an artifact of the fluorescent markers (Additional

file 4B-D).We observe that patterns of wave collisions are similar in habitats on the same device (i.e. habitats inoculated with cells from the same set of initial cultures; compare Figure 2B with D and C with E), however, there is a large variation in the collision patterns

between habitats on different devices inoculated with cells from a different set of initial MEK inhibitor drugs click here cultures (Figure 3). For each wave the post-collision outcome can be decomposed in three components: (i) part of the wave is reflected back, continuing to travel as a wave after quickly (within 10 min) having Angiogenesis inhibitor reversed its direction; (ii) part of the wave disintegrates and a local (sessile) population is formed; (iii) part of the wave is ‘refracted’, continuing to travel as a wave in the same direction as before the collision, although typically with a lower velocity. The distribution of bacteria from the incoming wave over these three components second can vary strongly between devices, as can be seen in Figure 3. For example: in Figure 3A the green and red α-waves both have strong reflected parts (49% and 29% of the cells in the red and green α-waves, respectively), in Figure 3B the red α-wave completely disintegrates and in Figure 3C a large part (46%) of the red α-wave is refracted.

The patterns can become more complex if subsequent incoming waves interact with the subpopulations formed in the initial collision. For example in Figure 3C, a red β-wave merges with a green stationary populations and a combined, two-strain wave (yellow), is formed and starts traveling to the left of the habitat. Figure 2 The collisions of colonization waves. (A) Occupancy measure (area fraction) calculated per patch for strains JEK1037 (red) and JEK1036 (green) showing the collision between two α waves (at t = 6 h, patch 54). Note how both waves branch: a part of the wave is reflected, a part forms a stationary population, and a part continuous (for a short distance) in the same direction. (B) Kymograph of fluorescence intensity for the collision shown in A. (C) Enlarged view of B, centered at the point of collision. Note how the red and green populations remain largely segregated in space, even though individual cells do mix with the other population. (D) Kymograph of fluorescence intensity of a collision in a different habitat in the same device (with separate inlets; type-2) as the habitat shown in A- C. Note the similarity between B and D.

This may be due to the disorder (amorphous nature) present in the

This may be due to the disorder (amorphous nature) present in the films. This peak also shows a slight blueshift with the increase in Cd content. Therefore, the peak observed at 425 nm agrees well with that of the reported results [40]. Figure 4 Photoluminescence spectra at various concentrations of Cd in thin films of a-(PbSe) 100−x Cd

x nanoparticles. The understanding of optical and electrical processes in lead chalcogenide materials in nanoscale is of great interest for both fundamental and technological points of view. In recent years, owing to their very interesting physical properties, this particular material has raised a considerable deal of research interest followed by technological applications in the field BIIB057 supplier of micro/optoelectronics. Significant research efforts have

been focused to the study of the optical and electrical properties of this KU-57788 cost compound in thin film formation because the optimization of device performance requires a well-established knowledge of these properties of PbSe and metal-doped PbSe thin films. Here, we have studied the optical absorption, reflection, and transmission of amorphous thin films of (PbSe)100−x Cd x nanoparticles as a function of the incident wavelength in the range of 400 to 1–200 nm. The optical absorption studies of materials provide a simple approach to understand the band structure and energy gap of nonmetallic materials. Normally, the absorption coefficient is measured in the high and intermediate absorption regions to study the optical properties of materials.

It is one of the most important means of determining the band structures of semiconductors. On the basis of measured optical density, Vorinostat cell line we use the following relation to estimate the values of the absorption coefficient [4]: (1) where OD is the optical density measured at a given layer thickness (t). On the basis of the calculated values of absorption coefficient, we have observed that the value of absorption coefficient increases with the increase in photon energy for all the studied thin films of a-(PbSe)100−x Cd x nanoparticles. During the absorption MLN2238 price process, a photon of known energy excites an electron from a lower to a higher energy state, corresponding to an absorption edge. In the case of chalcogenides, we observe a typical absorption edge, which can be broadly attributed to one of the three processes: (1) residual below-gap absorption (2) Urbach tails, and (3) interband absorption. Highly reproducible optical edges are being observed in chalcogenide glasses. These edges in chalcogenides are relatively insensitive to the preparation conditions, and only the observable absorption [41] with a gap under equilibrium conditions accounts for the first process.

Cells attached to the flasks were treated with 100 nmol/L gefitin

Cells attached to the flasks were treated with 100 nmol/L gefitinib, meanwhile, irradiated with graded doses of x-rays, rinsed after 48-hour incubation in drug-containing medium, and allowed to form colonies in drug-free medium. Surviving fractions for radiation + MK0683 gefitinib were normalized by dividing by the surviving fraction for gefitinib only. Each test was performed 3 times. The radiation-enhancing (t = 7.65, P < 0.01) effect of gefitinib was comparable with that of gefitinib alone in H-157 cells. (B) Effects of gefitinib on H-157 cell growth after irradiation. There was no significant difference (t = 1.13, P > 0.05) in the growth rates between H-157 cells and gefitinib-treated

cells as determined by cell counting, but the proliferative ability check details of the gefitinib and radiation treated cells was dramatically suppressed(t = 5.01, P < 0.05)in contrast with radiation-treated only. Gefitinib increased the radiation-induced apoptosis As shown in Figure 5. The early apoptosis rate among gefitinib-treated H-157 cells after 6 Gy irradiation was significantly higher than the cells with the same dosage of X-rays only. Whereas, no significant apoptotic changes were observed in unirradiated cells before and after gefitinib treated. Quantitative measurements of apoptotic cell

death by FCM in H-157 cells sufficiently indicated that the radiation-induced overexpression of PTEN significantly enhanced gefitinib-induced apoptosis in comparison GSK1904529A research buy with that of the control (no irradiation). Figure 5 Gefitinib-induced apoptosis in H-157 cells before and after irradiation. Attached cells were exposed to 6 Gy irradiation and then treated with 100 nmol/L gefitnib. After additional 48-hour incubation

in medium containing the drugs, the cells were harvested. The apoptotic index (AI) was measured using flow cytometry. (A) Control groups (AI: 1.36 ± 0.74%). (B) Apoptotic values after treatment with 100 nmol/L gefitinib alone (AI:3.58 ± 0.61%).(C) Radiation- induced apoptosis induction (14.26 ± 2.97%% of total cells) in H-157 cells.(D) Radiation combined with gefitinib induced apoptosis induction (23.58 ± 3.61% of total cells). Apoptotic values were normalized by subtracting control values; Urease the normalized apoptotic values were used for statistical analyses. Experiments were done in triplicate. Combined drug treatments were shown to enhance radiation-induced apoptosis in H-157 cells (t = 19.91, P < 0.01), but no synergistic manner when compared with drug alone without radiation (t = 2.569, P > 0.05). Discussion The PI3K pathway is a critical effector of growth, proliferation, and survival pathways. PTEN serves as negative regulator of the phosphatidylinositol 3-kinase (PI3K) pathway by removing the third phosphate from the inositol ring of the second messenger PIP3 [29]. PTEN inactivation results in accumulation of PIP3 levels and persistent signaling through the serine/threonine kinase Akt/protein kinase B.

Nat Nanotechnol 2008, 3:724–726 CrossRef 6 Shimizu T, Matsumoto

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W, Moon WJ, Tanaka E, Nutlin-3a nmr Otabe ES: Finite size effects on Néel temperature in antiferromagnetic nanoparticles. Phys Rev B 2005, 72:014464.CrossRef 13. White RM, Geballe TH: Long Range Order in Solids. New York: Academic; 1979. 14. Chrzanowski J, Irwin JC: Raman scattering from cupric oxide. Solid State Commun 1989, 70:11–14.CrossRef 15. Irwin JC, Chrzanowski J, Wei T, Lockwood DJ, Wold A: Raman scattering from single crystals of cupric oxide. Physica C 1990, 166:456–464.CrossRef 16. Cheng C-L, Ma Y-R, Chou MH, Huang CY, Yeh V, Wu SY: Direct observation of short-circuit Thiamet G diffusion during the formation of a single cupric oxide nanowire. Nanotechnology 2007, 18:245604.CrossRef 17. Rousseau DL, Bauman RP, Porto SPS: Normal mode determination in crystals. J Raman Spectrosc 1981, 10:253–290.CrossRef 18. Hagemann H, Bill H, Sadowski W, Walker E, Francçis M: Raman spectra of single crystal CuO. Solid State Commun 1990, 73:447–451.CrossRef 19. Goldstein HF, Kim DS, Yu PY, Bourne LC: Raman study of CuO single crystals. Phys Rev B

1990, 41:7192–7194.CrossRef 20. Campbell IH, Fauchet PM: The effects of microcrystal size and shape on the one phonon Raman spectra of crystalline semiconductors. Solid State Commun 1986, 58:739–741.CrossRef 21. Kliche G, Popovic ZV: Far-infrared spectroscopic investigations on CuO. Phys Rev B 1990, 42:10060–10066.CrossRef 22. Xu JF, Ji W, Shen ZX, Li WS, Tang SH, Ye XR, Jia DZ, Xin XQ: Raman spectra of CuO nanocrystals. J Raman Spectrosc 1999, 30:413–415.CrossRef 23. Balkanski M, Wallis RF, Haro E: Anharmonic effects in light scattering due to optical phonons in silicon. Phys Rev B 1983, 28:1928–1934.CrossRef 24. Lockwood DJ, Gottam MG: The spin‒phonon interaction in FeF 2 and MnF 2 studied by Raman spectroscopy. J Appl Phys 1988, 64:5876.CrossRef 25.