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1.
检测了阿司匹林对照品与肠溶片的常规拉曼光谱和表面增强拉曼光谱,归属了各个振动峰位和增强峰位;研究了阿司匹林溶液与DNA相互作用的表面增强拉曼光谱与紫外光谱。结果表明:阿司匹林对照品与肠溶片的NRS及SERS图谱基本一致,药品的辅料对阿司匹林的检测几乎没有影响;在SERS中,阿司匹林分子是通过羧基和苯环垂直吸附在纳米银表面;阿司匹林分子与DNA相互作用的主要键合模式是插入作用,阿司匹林中的苯环和CO插入到DNA双螺旋结构的碱基对之间,为深入了解此类药物的作用机理提供了十分重要的信息和有益的参考。  相似文献   

2.
对炔基苯硫酚分子吸附在银纳米粒子上表现出较强的表面增强拉曼光谱(SERS)信号。本文采用密度泛函理论(DFT)对炔基在银纳米粒子上不同吸附方式以及振动光谱进行了计算分析。研究结果表明,当炔基与金属之间有相互作用时,C≡C键伸缩振动的频率红移,拉曼强度显著增强。同时也从分子与金属作用角度初步探讨了实验所观测谱线宽度增宽的现象。此外,通过含时密度泛函理论(TD-DFT)进一步研究了吸附分子与金属之间的电荷转移性质,并分析了其预共振拉曼光谱。该工作初步建立了在银表面上炔键的吸附构型与SERS光谱之间的关系。  相似文献   

3.
用硝酸腐蚀法处理得到了具有表面增强拉曼光谱 (SERS)活性的银表面。在表面温度于 - 1 90℃~30℃变化时 (上升和下降 ) ,分别测定了吸附在银表面上的腺嘌呤、嘌呤和四并苯的表面增强拉曼光谱 ,观察到一系列有关拉曼峰频率和强度的可逆变化。结果表明 ,温度降低 ,吸附分子SERS中受电磁增强机制作用的振动的拉曼位移发生蓝移 ,同时峰强度也有变化 ;而受化学增强机制作用的振动的拉曼位移则不受温度的影响。温度的变化导致分子平面可弯曲分子在金属表面的取向发生变化 ,如腺嘌呤和嘌呤在高温下取直立态 ,而平面的对称分子 (如四并苯 )在表面上的取向则不受温度的影响。  相似文献   

4.
报道了阿莫西林对照品与阿莫西林胶囊的常规拉曼光谱(NRS)和在银胶基底上溶液的表面增强拉曼光谱(SERS),归属了各个振动峰位和增强峰位;研究了阿莫西林对照品溶液与DNA相互作用的荧光光谱和表面增强拉曼光谱.结果表明:阿莫西林胶囊与阿莫西林对照品的NRS及SERS图谱基本一致,说明胶囊中的辅料对阿莫西林的检测几乎没有影...  相似文献   

5.
利用拉曼光谱仪测定L-半胱氨酸(L-Cys)的常规拉曼光谱(NRS)和表面增强拉曼光谱(SERS),发现L-Cys在纳米银棒上有明显的拉曼增强效应,对分子特征峰进行了归属,研究L-Cys在银纳米棒基底表面吸附机理,在固体NRS中在2 576 cm-1出处有明显的S-H伸缩振动峰,而SERS中没有出现,实验表明纳米银棒与L-Cys巯基上的S原子形成了Ag-S键,C-O和C-N伸缩振动有明显的增强。在不同pH值条件下,分析了L-Cys的拉曼光谱差异,探讨吸附行为的变化。在pH值为6时,S-H的伸缩振动峰基本消失,形成了稳定的S-Ag键;随着pH值增加趋于碱性时,羧基易失去H原子形成-COO-易与银发生吸附作用且振动峰增强。在pH值为7时,S原子与Ag形成稳定的S-Ag键,C-O和C-N的振动峰也最稳定。选择在pH值为7的条件下,在L-Cys溶液中加入Na+,Mg2+和Cu2+ 等10种金属盐,发现Al3+,Cu2+,Zn2+,Cd2+和Hg2+ 使L-Cys分子的结构发生了改变,金属离子与L-Cys另一端羧基发生作用,其中Cu2+,Zn2+,Cd2+和Hg2+随半径增大与S原子的孤电子发生作用越大。探讨了在不同pH值、不同比例和不同浓度下,金属离子与L-Cys作用SERS的变化,随着pH值、比例和浓度的增大,峰的强度有减小趋势。Cu2+与L-Cys作用的SERS信号很弱,Hg2+与L-Cys作用只出现了一个C-O的振动峰,说明Hg2+完全破坏了L-Cys的空间构型。该研究对蛋白质变性等的研究提供了重要参考信息。  相似文献   

6.
采用二维相关红外光谱方法研究了4-氨基吡啶和甲基丙烯酸分子问相互作用.一维红外光谱难以直接反映4-氨基毗啶和甲基丙烯酸分子间相互作用的类型和键的关联,而二维相关分析结果清晰表明4-氨基吡啶和甲基丙烯酸分子间存在的相互作用.研究中发现1298和1 202 cm-1归属于甲基丙烯酸的-OH伸缩振动峰与1 531 cm-14-氨基吡啶的C=N伸缩振动峰存在同步交叉正峰,3 382和3 212 cm-1属于4-氨基吡啶的氨基N-H伸缩振动峰与1 705 cm-1归属于甲基丙烯酸的羰基伸缩振动峰存在同步交叉正峰.根据二维相关规则,4-氨基吡啶的C=N峰与甲基丙烯酸的-OH峰、4-氨基吡啶的氨基N-H峰与甲基丙烯酸的羰基峰有很强协同作用.结果表明4-氨基吡啶的C=N与甲基丙烯酸的-OH存在静电作用,4-氨基吡啶的氨基与甲基丙烯酸的羰基存在氢键作用.二维红外光谱是研究分子内、分子间相互作用的一种强有力的手段.  相似文献   

7.
本文采用杂化密度泛函理论计算了过渡金属M -Py分子的基态振动频率和拉曼光谱强度。计算结果表明过渡金属对Py分子的振动频率影响较小 ,但对Py分子的A1 振动模式的拉曼谱强度影响较大。对于A1 对称性的非C -H伸缩振动模 ,吡啶分子环呼吸振动和高频的C -C对称伸缩振动有较大的拉曼散射因子 ,我们还将此结果与典型的SERS活性金属 (铜族金属 )进行了比较  相似文献   

8.
在银电极表面形成一层C60薄膜,分别在乙腈溶液和水溶液中进行表面增强拉曼光谱(SERS)研究并将两者进行比较,从而消除了溶液中的C60干扰表面吸附C60的SERS谱图的可能性.研究结果表明,C60分子对称性的降低导致SERS谱峰发生了分裂;表面电磁场的作用使得光谱选律在SERS效应中被拓宽,产生了新的拉曼谱峰.该结果与团簇吸附在粗糙银电极表面的C60分子的研究结果相似.与之不同的是在乙腈溶液和水溶液中的SERS谱图的低波数区内分别在348和311 cm-1左右出现一个新峰,经过分析可认为该峰与C60-金属基底的相互作用有关.  相似文献   

9.
小檗碱在TLC原位的FT-SERS研究   总被引:4,自引:0,他引:4  
应用表面增强技术将薄层色谱与近红外傅里叶变换拉曼光谱联用,获得了中成药三黄片中主要有效成分小檗碱在薄层原位的傅里叶变换表面增强拉曼光谱(FT-SERS)。研究表明,在薄层原位约2.5μm样品的FT-SERS与纯固体样品的FT-Raman光谱的主要特征峰波数基本一致,相对强度有一定变化,出现特别增强的拉曼峰是波数为727nm的芳香环上CH键面内变形振动峰。小檗碱分子以异喹啉环共轭体系的π电子与表面增强活性物质银晶体微粒相互作用,呈平面吸附样式。获得了中成药三黄片中主要有效成分小檗碱分离与高灵敏度指纹检测的可靠的新方法。  相似文献   

10.
AMP和DNA的银溶胶增强拉曼光谱   总被引:6,自引:0,他引:6  
本文报道了生物分子5‘-腺苷磷酸(AMP)和脱氧核糖核酸(DNA)在银溶胶中的增强拉曼光谱。实验结果表明用银溶胶增加方法可以得到在较低浓度下、几乎不受光干扰的增强拉曼光谱。与固体AMP和DNA拉曼光谱进行比较,发现谱峰有很好的一致性,但也存在差异,如对应于固体AMP中715cm^-1处的腺嘌呤的呼吸振动峰加强,并位移到723cm^-1处,813cm^-1处的磷酸酯的对称伸缩振动峰消失了;在DNA中核糖环的振动峰明显加强,A,T,C,G四种碱基的峰也得到了不同程度的增强。通过对实验结果的分析,推测了AMP和DNA在银溶胶界面的吸附状态和分子结构。  相似文献   

11.
Raman spectra of the Cl3CCHO/CCl4 and Cl3CCHO/C6D12 binary systems were recorded as a function of the mole fraction. Features originating from self‐aggregates of chloral (trichloroethanal, trichloroacetaldehyde—TCAA) molecules were detected in different spectral regions. The most pronounced changes were observed in the vicinity of the ν(CO) and ν(C H) stretching vibration bands. Using two‐dimensional correlation spectroscopy (2D‐COS), evolving‐factor analysis (EFA) and multivariate curve resolution (MCR), dimer bands were identified, and their positions were determined. The ν(C H) stretching vibration band in dimers was blue‐shifted by nearly 18 cm−1, whereas the ν(CO) dimer band was red‐shifted by more than 5 cm−1. For these bands, the observed shifts were accompanied by an almost twofold change in the bandwidth, from approximately 19 and 6 cm−1 for dilute solutions (x = 0.05) to 36.6 and 11.5 cm−1, respectively, in pure TCAA. The formation of dimers was confirmed by multivariate analysis of the Raman spectra of chloral recorded as a function of temperature. Analogous analysis of dichloroacetyl chloride (DCAC) spectra gave an 8.9 cm−1 blue shift for the ν(C H) vibration band and − 5.5/− 10.1 cm−1 shifts for the ν(CO) stretching vibrations of the two conformers present. To facilitate the interpretation of experimental findings, the optimized geometries and vibrational wavenumbers of the Cl3CCHO/HCl2CCClO molecules and (Cl3CCHO)2/(HCl2CCClO)2 dimers were calculated at the B3LYP/6‐311 + + G(3df,3pd) level. Copyright © 2010 John Wiley & Sons, Ltd.  相似文献   

12.
Fourier‐transform infrared (FT‐IR), Raman (RS), and surface‐enhanced Raman scattering (SERS) spectra of β‐hydroxy‐β‐methylobutanoic acid (HMB), L ‐carnitine, and N‐methylglycocyamine (creatine) have been measured. The SERS spectra have been taken from species adsorbed on a colloidal silver surface. The respective FT‐IR and RS band assignments (solid‐state samples) based on the literature data have been proposed. The strongest absorptions in the FT‐IR spectrum of creatine are observed at 1398, 1615, and 1699 cm−1, which are due to νs(COOH) + ν(CN) + δ(CN), ρs(NH2), and ν(C O) modes, respectively, whereas those of L ‐carnitine (at 1396/1586 cm−1 and 1480 cm−1) and HMB (at 1405/1555/1585 cm−1 and 1437–1473 cm−1) are associated with carboxyl and methyl/methylene group vibrations, respectively. On the other hand, the strongest bands in the RS spectrum of HMB observed at 748/1442/1462 cm−1 and 1408 cm−1 are due to methyl/methylene deformations and carboxyl group vibrations, respectively. The strongest Raman band of creatine at 831 cm−1w(R NH2)) is accompanied by two weaker bands at 1054 and 1397 cm−1 due to ν(CN) + ν(R NH2) and νs(COOH) + ν(CN) + δ(CN) modes, respectively. In the case of L ‐carnitine, its RS spectrum is dominated by bands at 772 and 1461 cm−1 assigned to ρr(CH2) and δ(CH3), respectively. The analysis of the SERS spectra shows that HMB interacts with the silver surface mainly through the  COO, hydroxyl, and  CH2 groups, whereas L ‐carnitine binds to the surface via  COO and  N+(CH3)3 which is rarely enhanced at pH = 8.3. On the other hand, it seems that creatine binds weakly to the silver surface mainly by  NH2, and C O from the  COO group. Copyright © 2006 John Wiley & Sons, Ltd.  相似文献   

13.
The strength and geometry of adsorption of substituted propenoic acids on silver surface were studied by means of surface enhanced Raman spectroscopy (SERS) using silver sol. Based on their SERS behavior, two classes of phenylpropenoic acids studied were distinguished. The first class of propenoic acids (atropic acid, (E)‐2,3‐diphenylpropenoic acid, (E)‐2‐(2‐methoxyphenyl)‐3‐phenylpropenoic acid, (E)‐2,3‐di‐(4‐methoxyphenyl)phenylpropenoic acid and (E)‐2‐(2‐methoxyphenyl)‐3‐(4‐fluorophenyl)propenoic acid) has shown strong charge transfer (CT) effect. We suggest bidentate carboxyl bonded species based on the SERS enhanced bands of νCOO around 1394 cm−1 and νC―C of the ―C―COO moiety at 951 cm−1. In these series the plane of the α‐phenyl group (γCH out‐of‐plane vibrations at 850–700 cm−1) is almost parallel to the silver surface, while the β‐phenyl group is in tilted position depending on the type and the position of substituent(s) showing strong SERS enhanced bands of νCC + βCH (in‐plane mode) at 1075 cm−1, νCC (ring breathing mode, in‐plane) at 1000 cm−1 and γCCC (out‐of‐plane mode) around 401 cm−1. The other class of propenoic acids (cinnamic acid, (E)‐2‐phenyl‐3‐(4‐methoxyphenyl)propenoic acid) has shown weak electromagnetic (EM) enhancement (CC bands is enhanced in cinnamic acid). In this case no significant carboxyl enhancement was observed, so we suggest that adsorbed species lie parallel to the surface. The two types of adsorption can be related to the dissociation ability of the carboxylic group. In the first case the carboxylic H dissociates, while in the second case it does not, as indicated also by the characteristic νCO band at 1686 cm−1 in the FT‐Raman spectra of methanolic solutions. Copyright © 2015 John Wiley & Sons, Ltd.  相似文献   

14.
The Surface‐enhanced Raman scattering of benzenesulfonamide and sulfanilamide adsorbed on silver sols was studied. On the basis of the noticeable shifts observed for wavenumbers of the νs(OSO), ν(CS), and ν(SN) vibrations with respect to the Raman spectra of the solids and the ionic solutions, we conclude that these molecules are adsorbed on silver nanoclusters at pH ≥ 7 with the aminosulfonyl groups partially deprotonated. The benzenesulfonamide links to the metal through the nitrogen atom of the corresponding azanion, while the sulfanilamide interacts in turn through the nitrogen atoms of the –NH2 and –SO2NH groups in the para‐position. Additionally, it was found that the most enhanced surface‐enhanced Raman scattering bands, especially the 8a;νring mode, are related to the presence of the charge transfer mechanism. Copyright © 2011 John Wiley & Sons, Ltd.  相似文献   

15.
偶氮类化合物热相变动态过程的二维相关拉曼光谱研究   总被引:1,自引:0,他引:1  
利用变温傅里叶变换拉曼光谱(FT-Raman)研究含偶氮苯基长链脂肪酸化合物8A5H固体的热相变。二维相关光谱分析技术被应用到以温度为变量的同步和异步相关计算,目的在于研究该化合物中不同基团在热相变过程中取向变化过程以及变化趋势、步骤等一系列的动态结构变化。展示了研究偶氮类化合物热致相变过程中结构动态新的研究方法,同时也为二维相关光谱的应用拓宽了新的研究领域。  相似文献   

16.
Eritadenine, 2(R),3(R)‐dihydroxy‐4‐(9‐adenyl)‐butyric acid, is a cholesterol‐reducing compound naturally occurring in the shitake mushroom (Lentinus edodes). To identify the unknown Raman spectrum of this compound, pure synthetic eritadenine was examined and the vibrational modes were assigned by following the synthesis pathway. This was accomplished by comparing the known spectra of the starting compounds adenine and D ‐ribose with the spectra of a synthesis intermediate, methyl 5‐(6‐Aminopurin‐9H‐9‐yl)‐2,3‐O‐isopropylidene‐5‐deoxy‐β‐D ‐ribofuranoside (MAIR) and eritadenine. In the Raman spectrum of eritadenine, a distinctive vibrational mode at 773 cm−1 was detected and ascribed to vibrations in the carbon chain, ν(C C). A Raman line that arose at 1212 cm−1, both in the Raman spectrum of MAIR and eritadenine, was also assigned to ν(C C). Additional Raman lines detected at 1526 and at 1583 cm−1 in the Raman spectrum of MAIR and eritadenine were assigned to ν(N C) and a deformation of the purine ring structure. In these cases the vibrational modes are due to the linkage between adenine and the ribofuranoside moiety for MAIR, and between adenine and the carbon chain for eritadenine. This link is also the cause for the disappearance of adenine specific Raman lines in the spectrum of both MAIR and eritadenine. Several vibrations observed in the spectrum of D ‐ribose were not observed in the Raman spectrum of eritadenine due to the absence of the ribose ring structure. In the Raman spectrum of MAIR some of the D ‐ribose specific Raman lines disappeared due to the introduction of methyl and isopropylidene moieties to the ribose unit. With the approach presented in this study the so far unknown Raman spectrum of eritadenine could be successfully identified and is presented here for the first time. Copyright © 2008 John Wiley & Sons, Ltd.  相似文献   

17.
The mineral wheatleyite has been synthesised and characterised by Raman spectroscopy complimented with infrared spectroscopy. Two Raman bands at 1434 and 1470 cm−1 are assigned to the ν(C O) stretching mode and implies two independent oxalate anions. Two intense Raman bands observed at 904 and 860 cm−1 are assigned to the ν(C C) stretching mode and support the concept of two non‐equivalent oxalate units in the wheatleyite structure. Two strong bands observed at 565 and 585 cm−1 are assigned to the symmetric CCO in plane bending modes. The Raman band at 387 cm−1 is attributed to the CuO stretching vibration and the bands at 127 and 173 cm−1 to OCuO bending vibrations. A comparison is made with Raman spectra of selected natural oxalate bearing minerals. Oxalates are markers or indicators of environmental events. Oxalates are readily determined by Raman spectroscopy. Thus, deterioration of works of art, biogeochemical cycles, plant metal complexation, the presence of pigments and minerals formed in caves can be analysed. Copyright © 2008 John Wiley & Sons, Ltd.  相似文献   

18.
使用太赫兹时域光谱(THz-TDS)、傅里叶红外光谱(FTIR)和傅里叶拉曼光谱(FT-Raman)技术在室温下对γ-氨基丁酸(GABA)、苯甲酸(BA)及其研磨和溶剂共晶体进行表征分析。FTIR,FT-Raman及THz光谱都能够分辨原料物质及GABA-BA共晶体。其中THz实验结果显示了GABA-BA研磨和溶剂共晶体位于0.93,1.33,1.57THz的吸收峰明显区别于原料物质,这体现了不同物质在THz波段具有明显的指纹特征。为确认GABA-BA共晶体的晶型结构,分别采用FTIR和FT-Raman光谱进行光谱归属。通过FTIR的光谱归属推断GABA-BA共晶体由GABA中的氨基H_23和BA中的羰基O1构成第一个氢键,氨基中的N18结合BA中的羟基H15形成第二个氢键。FT-Raman光谱中,原料物质GABA中位于576,886,1 250,1 283,1 337,1 423和1 470cm~(-1)处归属于—CH_2,—NH_2弯曲振动的Raman散射峰在GABA-BA共晶体内消失,判定GABA中的氮原子N18亦可作为氢键受体,从而验证了GABA-BA共晶体的晶型结构。此外,为了进一步说明溶剂pH值对GABA-BA共晶体的形成条件的影响,利用THz-TDS,FT-Raman光谱确认了该共晶体在溶剂条件2.00≤pH≤7.20可稳定地生成。这一研究结果同时也为利用THz-TDS,FTRaman光谱技术辨别固体物质晶型结构、晶型形成条件提供了实验及理论依据。  相似文献   

19.
Pigments from red coral (Corallium rubrum) and African snail (Helixia aspersa) shell were studied non‐invasively using Raman spectroscopy with 1064‐nm laser beam. The two observed bands because of organic pigments confined in biomineralized CaCO3 matrix at about 1500 and 1100 cm−1 were assigned to ν(CC) and ν(C―C), respectively. Both signals originate from polyene(s) of largely unknown structure, containing several conjugated CC bonds. The small peak at 1016 cm−1 in the Raman spectrum of coral pigment was assigned to in‐plane ―CH3 rocking or structural deformation of polyene chain because of spatial confinement in the mineral matrix. The organic pigments in red coral and snail shell were present in inorganic matrix containing aragonite (shell) and calcite (coral). In addition, using Raman spectroscopy, it was observed that aragonite was replaced by calcite as result of healing damaged parts of snail shell. This is an important finding which indicates a great potential of nondestructive Raman spectroscopy instead of X‐ray technique, as a diagnostic tool in environmental studies. To support analysis of the observed Raman spectra detailed calculations using density functional theory (DFT with B3LYP and BLYP density functionals) on structure and vibrations of model all‐trans polyenes were undertaken. DFT calculated CC and C―C stretching frequencies for all‐trans polyenes containing from 2 to 14 CC units were compared with the observed ν(CC) and ν(C―C) band positions of the studied coral and shell. Individual correction factors were used to better match theoretical wavenumbers with observed band positions in red coral and African snail. It was concluded that all‐trans polyene pigments of red coral and dark parts of African snail shell contain 11–12 and 14 CC double bond units, respectively. However, Raman spectroscopy cannot produce any clear information on the presence and nature of the end‐chain substituents in the studied pigments. Copyright © 2016 John Wiley & Sons, Ltd.  相似文献   

20.
The Raman spectra of 3‐(pent‐1‐enyl) methyl ether (3‐methoxypent‐1‐ene) and four deuterium‐labelled analogues are reported and discussed. Correlations between specific structural features and the associated Raman bands are developed, with a view to enhancing the analytical application of Raman spectroscopy in investigating materials containing an alkenyl group. Particular attention is given to developing means of distinguishing the methyl group attached to the carbon skeleton from that of the methoxy group, to maximize the analytical utility of the signals associated with ν(sp2 CH), ν(sp2 CH2) and ν(CC) stretching vibrations, and to interpreting in more detail certain δ(sp2 CH) and δ(sp2 CH2) vibrations of the atoms of the double bond. These results establish a definitive spectroscopic protocol for differentiating a methoxy group from a methyl substituent attached directly to a carbon atom in unsaturated ethers. Copyright © 2007 John Wiley & Sons, Ltd.  相似文献   

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