Vacuum-ultraviolet circular dichroism study of oligosaccharides using a synchrotron-radiation spectrophotometer

Abstract

Vacuum-ultraviolet circular dichroism (VUVCD) spectra of malto-, laminari-, isomalto-, and cello-oligosaccharide series and their corresponding polysaccharides (laminarin and dextran) were measured from 200 to 168 nm in aqueous solution at 25°C using a synchrotron-radiation VUVCD spectrophotometer. Disaccharides exhibited markedly different CD spectra depending on the types of glycosidic linkages, and the CD spectra of each oligosaccharide series (with the exception of the isomalto-oligosaccharide series) varied with the chain length below 190 nm while retaining the spectral shape of the constituent disaccharide. These results indicate that the basic structures of oligosaccharides were greatly affected by the configurations of their constituent disaccharides, which had unique torsion angles restricted by the intramolecular hydrogen bonds between glucose units. Based on comparisons between the experimental and theoretical data, we suggest that the chain-length dependence of CD above 180 nm reflects the backbone structure of oligosaccharides (e.g., helical structures), while those below 180 nm are influenced by other factors associated with higher-energy chromophores such as the hydroxyl groups. The reported comprehensive VUVCD spectra provide basic information for understanding the complicated structures of oligosaccharides in aqueous solution that can be used in their theoretical assignments.

Keywords

Chain-length dependence glycosidic linkage helical structure oligosaccharide vacuum-ultraviolet circular dichroism synchrotron radiation

1. Introduction

Vacuum-ultraviolet circular dichroism (VUVCD) spectroscopy is a powerful tool for analyzing saccharide structures (especially unsubstituted saccharides) in aqueous solution [2,11,14] because they contain high-energy chromophores such as hydroxyl groups and acetal bonds whose n–σ* electronic transitions are only detectable in the vacuum-ultraviolet (VUV) region below 190 nm [1,3,17,24,25]. Some previous studies have found that the VUVCD spectra are sensitive to the equilibrium structures of monosaccharides in aqueous solution, such as the gauche (G) and trans (T) conformations of the hydroxylmethyl group at C-5, and the α- and β-anomer configurations of the hydroxyl group at C-1 [3,17,24,25]. However, since the pairwise relationships between the structures and VUVCD of monosaccharides remained unclear from these experimental results, we have recently measured the VUVCD spectra of various methyl aldopyranosides including methyl α-d-glucopyranosides in aqueous solution [19,20] using a synchrotron-radiation (SR) VUVCD spectrophotometer at the Hiroshima Synchrotron Radiation Center [21,28]. Using the time-dependent density functional theory (TDDFT) and molecular dynamics (MD) simulations involving explicit water molecules [15,35,40], we theoretically revealed that the GT and GG rotamers exhibited negative and positive CD around 170 nm, respectively, while the α- and β-anomer configurations showed negative and positive CD around 160 nm, respectively [19,20]. These results indicate that the experimentally observed and theoretically calculated CD spectra of saccharides can be used to analyze the structures of not only monosaccharides but also more complicated saccharides such as oligosaccharides in aqueous solution.

Few VUVCD spectra of unsubstituted oligosaccharides including disaccharides have been reported, but interesting results have already been obtained, as well as for monosaccharides. Stipanovic et al. measured the CD spectrum of an isomalto-oligosaccharide series with an α-( $1 \to 6$ )-glycoside linkage between glucose units in aqueous solution down to 175 nm over average molecular weights ranging from 410 to 303,000 [38]. They found that all compounds exhibited positive CD below 190 nm with similar molar ellipticities, showing that the CD spectra were not largely affected by increases in chain length. Lewis and Johnson measured the CD spectra of three malto-oligosaccharides with an α-( $1 \to 4$ )-glycoside linkage between glucose units (maltose, maltotriose, and maltoheptaose) in heavy water [16]. Their spectra exhibited negative CD around 190 nm and positive CD around 170 nm, and changed markedly as the chain length increased. However, there were no indications of a chain-length dependence of CD attributed to the formation of a helical structure [16], although amylose – which is a polysaccharide composed of maltose units – is known to have a helical conformation in solution [42,43]. Pfannemüller and Ziegast measured the CD spectra of some longer amylose oligosaccharides and showed that these oligomers can form a helical structure without marked changes in CD [14,31]. On the other hand, the CD spectrum of pustulan polysaccharide with an β-( $1 \to 6$ )-glycoside linkage between glucose units ( $average molecular weight \approx 10, 000$ ), as measured by Stipanovic and Stevens, exhibited a positive peak around 177 nm but a negative peak around 185 nm, with the pustulan solution turning into a gel over time at 10°C [37]. X-ray diffraction confirmed that the time dependence of this negative peak was attributable to the helical formation of pustulan in solution. The study of Stipanovic and Stevens made the first observations of the CD band around 180–190 nm, which is related to the formation of the helical structure [37]. However, the relationships between the conformations and VUVCD of oligosaccharides remain controversial due to the interpretation of the observed CD spectra in the VUV region not being entirely consistent or being assigned explicitly. Therefore, more comprehensive VUVCD spectra data obtained using an SR light source – which can provide a higher flux of photons in the VUV region compared to other experimental light sources [18,41] – are indispensable for understanding how the oligosaccharide structures in aqueous solution contribute to the measured CD spectra.

In the present study we measured the VUVCD spectra of the unsubstituted malto-, laminari-, isomalto-, and cello-oligosaccharide series down to 168 nm in aqueous solution at 25°C using a VUVCD spectrophotometer with an SR light source with the aim of clarifying the contributions of the different types of constituent disaccharides and increases in chain length to the structures and CD spectra of oligosaccharides. Table 1 and Fig. 1 respectively present the structural parameters and the chemical structures of disaccharide units of each oligosaccharide series. Although the types of glycosidic linkages differ between the series, all of them are composed of glucose units in order to simplify the comparisons among the CD spectra. To our knowledge, this is the first systematic investigation of the VUVCD of oligosaccharides in aqueous solution using an SR spectrophotometer.

Table 1
Structural parameters of the oligosaccharide series examined in this study

Oligosaccharide Monosaccharide unit Disaccharide unit Polymer Glycosidic linkage

Malto-oligosaccharide d-Glucose Maltose Amylose α-( $1 \to 4$ )

Laminari-oligosaccharide d-Glucose Laminaribiose Laminarin β-( $1 \to 3$ )

Isomalto-oligosaccharide d-Glucose Isomaltose Dextran α-( $1 \to 6$ )

Cello-oligosaccharide d-Glucose Cellobiose Cellulose β-( $1 \to 4$ )

Oligosaccharide	Monosaccharide unit	Disaccharide unit	Polymer	Glycosidic linkage
Malto-oligosaccharide	d-Glucose	Maltose	Amylose	α-( $1 \to 4$ )
Laminari-oligosaccharide	d-Glucose	Laminaribiose	Laminarin	β-( $1 \to 3$ )
Isomalto-oligosaccharide	d-Glucose	Isomaltose	Dextran	α-( $1 \to 6$ )
Cello-oligosaccharide	d-Glucose	Cellobiose	Cellulose	β-( $1 \to 4$ )

Fig. 1.

Chemical structures of disaccharide units of the malto-, laminari-, isomalto-, and cello-oligosaccharide series examined in this study.

2. Materials and methods

2.1. Materials

Malto-oligosaccharides ( $degree of polymerization [DP] = 2 – 7$ ), laminari-oligosaccharides ( $DP = 2 – 7$ ), isomalto-oligosaccharides ( $DP = 2 – 7$ ), and cello-oligosaccharides ( $DP = 2 – 4$ ) were obtained from Seikagaku Kogyo. Maltooctaose, maltononaose, and maltodecaose (for which $DP = 8$ , 9, and 10, respectively) were obtained from Elicityl. Laminarin from Laminaria digitata (average $molecular weight = 7, 700$ [5]) and two types of dextran from Leuconostoc mesenteroides (average $molecular weight = 5, 000$ or 670,000) were purchased from Sigma. High-pressure liquid chromatography analysis revealed that maltooctaose, maltononaose, and maltodecaose were contaminated with 23.4% maltopentaose and 2.1% maltohexaose, 7.6% maltooctaose and 0.8% maltopentaose, and 17% maltononaose and 1.2% maltooctaose, respectively, while the other samples were of high purity ( $> 98 %$ ). All of the samples could therefore be used without further purification. The sample solutions were freshly prepared by dissolving the saccharides in double-distilled water at concentrations of 1.0–8.0 w/v%, followed by incubation for 1 day to attain anomeric equilibrium. The concentration of each saccharide was determined by using a dry-weight gravimetric technique.

2.2. VUVCD measurements

The VUVCD spectra were measured from 200 to 168 nm at 25°C using the SR-VUVCD spectrophotometer. Details of the spectrophotometer and optical cell used are available elsewhere [21,28]. The path length of the CaF₂ optical cell was adjusted using a Teflon spacer to 10 μm for the measurements from 200 to 172 nm, while no spacer was used for measurements below 172 nm in order to reduce the absorption of light by water. The spectra obtained without the spacer were calibrated by normalizing the ellipticities to the spectra measured using a 10 μm spacer in the overlapping wavelength region from 200 to 172 nm. The path length of the cell without spacer was estimated to be 1.4 μm by this calibration method [19,20]. All spectra were recorded with a 1.0-mm slit, 4-s time constant, 20-nm/min scan speed, 0.067-nm data interval, and 4–9 accumulations. The molar ellipticity (θ) of all saccharides was calculated using the molecular weight per monosaccharide unit, in which the total molecular weight is divided by the number of monosaccharides. The obtained spectra were reproducible within 5%, and the errors were mainly attributable to noise in the signals and inaccuracies in the length of the light path. The error was approximately twofold higher below 170 nm, mainly due to the increased noise of the signals and inaccuracies in the length of the light path.

3. Results

Figure 2 show the VUVCD spectra of the malto-, laminari-, isomalto-, and cello-oligosaccharides measured in this study, respectively. Two dextran polysaccharides and one laminarin polysaccharide were also measured for comparisons, and these are described in the corresponding figures. These figures clearly show CD spectra only in the VUV region below 190 nm, indicating that VUVCD spectroscopy is a powerful tool for detecting the structures of oligosaccharides in aqueous solution. None of these spectra exhibited any concentration dependence, suggesting the absence of aggregations between the solutes within the concentration range examined (1.0–8.0 w/v%) and also meaning that sufficient signal can be detected in the wavelength region below 190 nm where the absorption of water becomes heavy [22].

Fig. 2.

VUVCD spectra of oligosaccharides in aqueous solution at 25°C (a) malto-oligosaccharide series (maltose, black; maltotriose, red; maltotetraose, green; maltopentaose, blue; maltohexaose, sky blue; maltoheptaose, pink; maltooctaose, violet; maltononaose, brown; and maltodecaose, dark green). The intensities of CD in the negative region were shown in the 10-fold spectra. (b) laminari-oligosaccharide series (laminaribiose, black; laminaritriose, red; laminaritetraose, green; laminaripentaose, blue; laminarihexaose, sky blue; and laminariheptaose, pink) and laminarin (violet). (c) isomalto-oligosaccharide series (isomaltose, black; isomaltotriose, red; isomaltotetraose, green; isomaltopentaose, blue; isomaltohexaose, sky blue; and isomaltoheptaose, pink) and dextran ( $DP \approx 31$ , violet; and $DP \approx 4, 000$ , brown). (d) cello-oligosaccharide series (cellobiose, black; cellotriose, red; and cellotetraose, green).

3.1. Malto-oligosaccharide

Maltose is a disaccharide that has an α-( $1 \to 4$ )-glycosidic linkage between two d-glucose molecules. Figure 2(a) exhibits the VUVCD spectra of nine malto-oligosaccharides ( $DP = 2 – 10$ ) from 200 to 168 nm. This study did not measure the VUVCD spectrum of amylose (which is a polysaccharide composed of maltose units; Table 1) because this polymer is relatively insoluble. The figure indicates that the oligosaccharides exhibited similar spectral shapes, with one negative CD peak around 190 nm and positive CD around 170 nm. Similar spectral characteristics were observed previously for maltose, maltotriose, and maltohexaose ( $DP = 2$ , 3, and 6) in heavy water [16], and in the present study we extended the number of glucose units of the oligosaccharides down to $DP = 10$ in order to clarify how the chain length contributes to the CD spectra. From this figure, the position and intensity of the negative CD peak around 190 nm observed for maltose exhibited a gradual blue shift and decrease, respectively, as the chain length increased. Further, the CD intensity below 180 nm also decreased gradually as the chain length increased.

To clarify how the malto-oligosaccharide spectra varied with the chain length, the CD intensity at the peaks at 190 and 170 nm (where maltose exhibited a negative CD peak and positive CD, respectively) are plotted against the DP in the inset of Fig. 2(a). It is evident that the peak intensity around 190 nm decreased exponentially as the DP increased, saturating at around $DP = 8$ , while the peak intensity around 170 nm continued decreasing. These results indicate that the CD at these two wavelengths (170 and 190 nm) reflect electronic transitions originating from different chromophores in oligosaccharides.

3.2. Laminari-oligosaccharide

Laminaribiose contains two d-glucose molecules joined by an β-( $1 \to 3$ )-glycosidic linkage, and laminarin is a polysaccharide composed of laminaribiose units. Figure 2(b) shows the VUVCD spectra of seven laminari-oligosaccharides ( $DP = 2 – 6$ ) and one laminarin polysaccharide. The VUVCD spectrum of laminaribiose had two positive peaks around 186 and 172 nm, and one negative peak around 177 nm. Laminaritriose exhibited one broad positive peak around 190 nm, one negative peak around 175 nm, and positive CD around 170 nm, which were close to the peak positions and CD sign for laminaribiose, although the intensities differed markedly around 175 nm. The VUVCD spectra of remaining four oligosaccharides (laminaritetraose, laminaripentaose, laminarihexaose, and laminariheptaose) had shapes similar to that for laminaritriose, but the negative peak around 177 nm decreased gradually as the number of glucose units increased, as also found for the malto-oligosaccharide series. Further, laminarin ( $DP \approx 45$ ) [5], which primarily comprises poly β-( $1 \to 3$ ) with some β-( $1 \to 6$ ) interstrand linkages and branch points, showed a negative peak around 174 nm with a larger intensity compared to laminaritriose.

The CD intensities at 186, 177, and 172 nm where laminaribiose exhibited CD peaks are plotted against the number of glucose units in the inset of Fig. 2(b). As for the malto-oligosaccharide series (Fig. 2(a)), the CD intensity decreased gradually as the chain length increased. A particularly interesting finding was that the intensities of the CD spectra of laminariheptaose and laminarihexaose at 186 nm were similar to that of laminarin, indicating that the intensity at this wavelength decreased exponentially and saturated around $DP = 6$ or 7, in comparison to there being only a small degree of saturation at 177 and 172 nm. These results show that the changes in the CD spectra with increases in chain length varied with the wavelength region (below or above 180 nm), as also found for the malto-oligosaccharide series (Fig. 2(a)).

3.3. Isomalto-oligosaccharide

Isomaltose contains two d-glucose molecules joined by an α-( $1 \to 6$ )-glycosidic linkage, and dextran is a polysaccharide composed of isomaltose units. Figure 2(c) shows the VUVCD spectra of five isomalto-oligosaccharides ( $DP = 2 – 6$ ) and two dextran polysaccharides from 260 to 170 nm. Although no CD peak was found for these oligosaccharides, all of the saccharides exhibited positive intensities below 190 nm. A particularly interesting finding was that the VUVCD spectra of all oligosaccharides with molecular weights from 342.3 to 1,153 were similar to those of two dextran polysaccharides with average molecular weights of 5,000 ( $DP \approx 31$ ) and 670,000 ( $DP \approx 4, 000$ ) for all wavelengths down to 170 nm. The CD intensity for the peaks at 185 and 170 nm are plotted against the DP in the inset of Fig. 2(c). This figure shows that there were no characteristic trends, implying the absence of chain-length dependence in the CD of isomalto-oligosaccharide series.

d-Glucose is a monosaccharide unit of isomalto-oligosaccharides that has equilibrium structures in aqueous solution such as the G/T conformers of the hydroxylmethyl group at C-5 and the α/β-anomers of the hydroxyl group at C-1. It is known that these structures affect the CD spectra below 190 nm [19,20]. The end reducing glucose units with α/β-anomer configurations might underlie the chain-length dependence of the CD spectra, because this effect should decrease gradually as the chain length increases. However, since the VUVCD spectra of isomalto-oligosaccharide series are mostly constant, this suggests negligible or only small contributions of the anomer to the VUVCD spectra down to 170 nm. Further, all of the oligosaccharide series examined in this study are composed of glucose units, and each oligosaccharide series has the same glycosidic linkage, and hence it can be assumed that the contributions of the hydroxylmethyl group at C-5 to CD spectra are largely similar within each oligosaccharide series. This assumption would be reasonable because the populations of G/T conformers of the constituent monosaccharides could be used to accurately calculate the optical rotations of certain disaccharides [9,36].

3.4. Cello-oligosaccharide

Cellobiose is a disaccharide with a β-( $1 \to 4$ )-glycosidic linkage between two d-glucose molecules. Cellulose is a polymer composed of cellobiose units and is relatively insoluble, resulting in cello-oligosaccharides above $DP = 5$ not dissolving in aqueous solution. Figure 2(d) shows the VUVCD spectra of three cello-oligosaccharides ( $DP = 2$ , 3, and 4), illustrating that the VUVCD spectrum of cellobiose had one positive peak around 174 nm, as also observed previously [16,17]. The CD spectra of polysaccharides with ( $1 \to 4$ )-glycosidic linkages in thin solid film were positive for the α-linkage (amylose) and negative for the β-linkage (cellulose) in the 164–172 nm and these features were also observed for the spectra of maltose and cellobiose in the 180–190 nm. In the present study we newly found that cellotriose and cellotetraose also exhibited one positive peak around 174 nm and that the peak intensity decreased as the DP increased, although we found no characteristic changes when plotting the CD intensity at 174 nm against DP, in contrast to the results observed for the malto- and laminari-oligosaccharide series; however, this difference is probably due to the small amount of data. The spectral shapes of these three oligosaccharides were mostly same without the CD intensity. These results indicate that the spectral features varied significantly as the chain length increased, depending on the types of oligosaccharides and probably also the types of constituent disaccharides.

4. Discussion

Our VUVCD measurements of oligosaccharides revealed that the VUVCD spectra exhibited characteristic peaks reflecting differences in the types and lengths of oligosaccharides, thereby demonstrating that VUVCD is sensitively affected by the structure of oligosaccharides. Further, the spectral shapes within each oligosaccharide series were highly similar and the change in the spectra with increases in chain length depended on the types of oligosaccharides or constituent disaccharides, suggesting that the structure of oligosaccharides is mainly determined by the configurations of the constituent disaccharides. Therefore, the disaccharide configurations would be useful for understanding the structures and CD spectra of oligosaccharide in aqueous solution.

4.1. Unique torsion angles of constituent disaccharides affect VUVCD spectra

The crystal structures of disaccharides investigated in this study were already determined by X-ray crystallography [30], showing that maltose, laminaribiose, and cellobiose formed the intramolecular hydrogen bonds between HO’-3…O-2, HO’-4…O-5, and HO’-3…O-5, respectively, while isomaltose did not participate in such bonding (Fig. 1). These intramolecular hydrogen bonds should directly affect the backbone torsion angles of glycosidic linkages. Actually, analyses of the torsion angles of these disaccharides using NMR and X-ray methods [6,29,32] revealed differences in the types of glycosidic linkages, such as ϕ and φ values of 96.8 and 105.2, respectively, for maltose, and $- 69.1$ and $- 109.1$ for laminaribiose in the crystal structures, where ϕ and φ are the dihedral angles of O₅–C₁–O₁– C_n’ and C₁–O₁–C_n’– $C_{n - 1}$ ’ ( $n = 3$ or 4), respectively (see Fig. 1). On the other hand, Best et al. found that isomaltose exhibited multiple low-energy minima, with more flexible and more extended conformations in water compared with maltose in the MD simulations and NMR relaxation experiments [4], indicating that the torsion angle of glycosidic linkages in isomaltose is rather variable.

In CD calculations of methyl D-aldopyranosides using the TDDFT method at the CAM-B3LYP/6-311++G** level, the molecular orbitals and rotational strengths related to the electronic transitions of the hydroxyl group, ring oxygen, and methoxy oxygen showed that the wavelength region around 180–170 nm was mainly assigned to the n-σ* transitions from the lone-pair orbital (n-orbital) to the σ*-orbital of ring oxygen and methoxy oxygen (or acetal bond), with only small contributions from hydroxyl groups [19,20]. Further, CD calculations of maltose, laminaribiose, isomaltose, and cellobiose based on their crystal structures [30] using TDDFT method at the CAM-B3LYP/6-311++G** level showed that the wavelength region around 180 nm included the electronic transitions originating from the acetal bond in glysocidic linkages. This theoretical results are supported by the experimental ones of several disaccharides and polysaccharides in which some characteristic CD peaks depended on the types of glycosidic linkages were found around 180–170 nm [14,17]. These results suggest that the unique torsion angles of maltose, laminaribiose, isomaltose, and cellobiose molecules could contribute to their spectral differences (Fig. 2) and also become important factors influencing the backbone structure of oligosaccharide because the spectral shapes within each oligosaccharide series were highly similar.

4.2. Characteristic structures of oligosaccharides affect VUVCD spectra

To understand the spectral change of oligosaccharides with increases in chain length, it is important if the structural changes of oligosaccharides occur at the level of the torsion angle of glycosidic linkages as the chain length increases. Sugiyama et al. determined the torsion angles of malto-oligosaccharides ( $DP = 2 – 7$ ) and short-chain amylose using two-dimensional NMR spectra [39]. They found that the torsion angles of glycosidic linkages in triose- tetraose-, and pentaose-oligomers differed slightly from those of longer oligomers, indicating these three oligomers exhibit intermediate configurations between maltose and amylose. These slight differences in the oligosaccharide structures should contribute to the spectral changes of VUVCD shown in Fig. 2(a). They further suggested that the short-chain amylose with a mean of 16 or 17 residues comprised almost 3 complete turns of the helical coil, meaning that this amylose could form a helical structure with 6 or 7 glucose residues per turn. Goldsmith et al. applied difference Fourier analysis to analyze the structure of maltoheptaose, and suggested that this molecule has a left-handed helical structure comprising 6.5 glucose residue per turn [13]. As shown in Fig. 2(a), the intensities for wavelengths above 180 nm decreased from $DP = 2$ to $DP = 7$ and saturated at around seven or eight glucose molecules, which is very consistent with the number of glucose residues per turn observed using X-ray and NMR methods.

Deslandes et al. reported that torsion angles ϕ and φ of β-( $1 \to 3$ )-d-glucan (laminarin) are similar (but not identical) to those of laminaribiose in crystal structures [8], suggesting the presence of slight differences in torsion angles among laminari-oligosaccharides. Further, X-ray diffraction and NMR methods suggested that laminarin is composed of three strands of the parallel right-handed helix, with six glucose residues per turn [33,44]. As shown in Fig. 2(b), as well as the malto-oligosaccharide series, the CD intensity at 186 nm saturated at around $DP = 6$ or 7. These CD and X-ray results indicate that the wavelength region above 180 nm reflects the formation of helical structures of laminari-oligosaccharides, since the helical structure of pustulan in the gel state was observed at 185 nm [37] and the region around 180 nm included the electronic transition originating from the acetal bond in glysocidic linkages. On the other hand, only slight saturation was observed at 177 and 172 nm as well as at 170 nm for the malto-oligosaccharide series, suggesting that the wavelength region below 180 nm would be affected by contributions from other factors such as the hydroxyl groups at C-2, C-3, and C-4, since the theoretical calculations predicted that these groups were assigned to the higher-energy chromophores compared to those of acetal bonds [19,20].

Shen et al. showed differences in backbone torsion angles between cellobiose [7] and cellotetraose [12] in crystal structures [34]. Dudley et al. measured the ¹³C NMR spectra of cello-oligosaccharides and revealed that the transformation of the cello-oligosaccharide spectrum into that of cellulose is definitely established for cellotetraose and complete for cellopentaose and higher oligomers [10]. Cellulose is known to form sheet structures in crystal form [26,27]. These results suggest the presence of differences in torsion angles among the cello-oligosaccharides as well as the malto- and laminari-oligosaccharide series. Although we could not measure the CD spectra of cello-oligosaccharides above $DP = 5$ in this study due to insolubility, these structural differences of cello-oligosaccharides observed using X-ray and NMR methods might underlie the CD spectral changes shown in Fig. 2(d).

Dextran is known to form random structures [23], while amylose and laminarin form helical crystal structures. Figure 2(c) shows that there was no characteristic dependence on increases in the chain length in the isomalto-oligosaccharide series and dextran, which suggests that this oligosaccharide series is similar to random structures. These flexible structures would be induced by the extended structure of isomaltose units without intermolecular hydrogen bonds between glucose units.

While the theoretical assignment of oligosaccharide CD spectra using the TDDFT method and MD simulations would be necessary for understanding the relationships between the structure and VUVCD (especially, below 180 nm) of oligosaccharides, the present comprehensive experimental data suggest that the chain length dependence observed in the VUVCD spectra of malto- and laminari-oligosaccharide series should reflect their characteristic structures such as helices, while the isomalto-oligosaccharide series does not show such CD changes due to its flexibility.

5. Conclusions

The VUVCD spectra of various oligosaccharide series suggested that the structure of an oligosaccharide is based on the configuration of the constituent disaccharides, with some oligosaccharides forming a helical structure as the chain length increases, affecting the CD spectra below 190 nm. Investigating the structural characteristics of oligosaccharides is not only inherently interesting but also an important step toward understanding the structure and dynamics of polysaccharides. The further accumulation of VUVCD data and their theoretical assignments is important for understanding the more detailed structures of oligosaccharides and their biological functions, which opens new fields in the structural biology of glycoconjugates.

Footnotes

Acknowledgements

This work was financially supported by Grant-in-Aids for Scientific Research from the Ministry of Education, Science, Sports, and Culture of Japan (No. 22870021 and No. 15KK0260 to K.M.) and by a grant from Kurata Memorial Hitachi Science and Technology Foundation.

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