Interfacial Molecular-level Structures of Polymers and Biomacromolecules Revealed via Sum Frequency Generation Vibrational Spectroscopy

Xu Li; Liang Ma; Xiaolin Lu

doi:10.3791/59380

JoVE Journal > Biochemistry

생화학

Interfacial Molecular-level Structures of Polymers and Biomacromolecules Revealed via Sum Frequency Generation Vibrational Spectroscopy

Published: August 13, 2019

doi:

10.3791/59380

Xu Li¹, Liang Ma¹, Xiaolin Lu¹

¹State Key Laboratory of Bioelectronics, School of Biological Science & Medical Engineering,Southeast University

Summary

Being comprehensively utilized, sum frequency generation (SFG) vibrational spectroscopy can help to reveal chain conformational order and secondary structural change happening at polymer and biomacromolecule interfaces.

Abstract

As a second-order nonlinear optical spectroscopy, sum frequency generation (SFG) vibrational spectroscopy has widely been used in investigating various surfaces and interfaces. This non-invasive optical technique can provide the local molecular-level information with monolayer or submonolayer sensitivity. We here are providing experimental methodology on how to selectively detect the buried interface for both macromolecules and biomacromolecules. With this in mind, interfacial secondary structures of silk fibroin and water structures around model short-chain oligonucleotide duplex are discussed. The former shows a chain-chain overlap or spatial confinement effect and the latter shows a protection function against the Ca²⁺ ions resulting from the chiral spine superstructure of water.

Introduction

Development of sum frequency generation (SFG) vibrational spectroscopy can be dated back to the work done by Shen et al. thirty years ago¹^,². The uniqueness of the interfacial selectivity and sub-monolayer sensitivity makes SFG vibrational spectroscopy appreciated by a large number of researchers in the fields of physics, chemistry, biology, and materials science, etc³^,⁴^,⁵. Currently, a broad range of scientific issues related to surfaces and interfaces are being investigated using SFG, especially for complex interfaces with respect to polymers and biomacromolecules, such as the chain structures and structural relaxation at the buried polymer interfaces, the protein secondary structures, and the interfacial water structures⁹^,¹⁰^,¹¹^,¹²^,¹³^,¹⁴^,¹⁵^,¹⁶^,¹⁷^,¹⁸^,¹⁹^,²⁰^,²¹^,²²^,²³^,²⁴^,²⁵^,²⁶.

For polymer surfaces and interfaces, thin-film samples are generally prepared by spin-coating to obtain the desired surfaces or interfaces. The problem arises due to the signal interference from the two interfaces of the as-prepared films, which leads to inconvenience for analyzing the collected SFG spectra²⁷^,²⁸^,²⁹. In most cases, the vibrational signal only from one single interface, either film/substrate or film/the other medium, is desirable. Actually, the solution to this problem is quite easy, namely, to experimentally maximize the light fields at the desirable interface and minimize the light fields at the other interface. Hence, the Fresnel coefficients or the local field coefficients need to be calculated via the thin film model and to be validated with respect to the experimental results³^,⁹^,¹⁰^,¹¹^,¹²^,¹³^,¹⁴^,¹⁵^,³⁰.

With the above background in mind, some polymer and biological interfaces could be investigated in order to understand fundamental science from the molecular level. In the following, taking three interfacial issues as examples: probing poly(2-hydroxyethyl methacrylate) (PHEMA) surface and buried interface with substrate⁹, formation of silk fibroin (SF) secondary structures on the polystyrene (PS) surface and water structures surrounding model short-chain oligonucleotide duplex¹⁶^,²¹, we will show how the SFG vibrational spectroscopy helps to reveal the interfacial molecular-level structures in connection to the underlying science.

Protocol

1. SFG experimental

Use a commercial picosecond SFG system (Table of Materials), which provides a fundamental 1064 nm beam with a pulse width of ~20 ps and a frequency of 50 Hz, based on an Nd:YAG laser.
Convert the fundamental 1064 nm beam into a 532 nm beam and a 355 nm beam by using second and third harmonic modules. Directly guide the 532 nm beam as an input light beam and generate the other input mid-infrared (IR) beam covering the frequency range from 1000 to 4000 cm^-1 through the optical parametric generation (OPG)/optical parametric amplification (OPA)/difference frequency generation (DFG) process.
Set the incident angles of two input beams to be 53° (IR) and 64° (visible), respectively, versus the surface normal.
To detect the polymer interfacial structures (either film/substrate interface or film/the other medium interface), use ssp (s-polarized sum-frequency beam, s-polarized visible beam and p-polarized infrared beam) and ppp polarization combinations.
To detect the interfacial protein secondary structures and water structures surrounding DNA, besides ssp and ppp, use chiral spp and psp polarization combinations were used.
To ensure the samples were not damaged, control the infrared and visible pulse energies to be ~70 and ~30 μJ, respectively. A schematic of the SFG process with the energy level diagram was shown in Figure 1. Figure 2 shows the SFG system in our clean room.

2. Fresnel coefficients

Use right-angle prisms as substrates for all the experiments discussed here. There exist two interfaces for a polymer film on the solid substrate, i.e., polymer surface in air and polymer/substrate interface. Both can generate SFG signals since inversion symmetry is broken at both interfaces. Therefore, a collected SFG spectrum is an interfered one. However, the local field coefficients or the Fresnel coefficients at the two interfaces can be adjustable by varying either the incident angles or the film thickness one at a time or simultaneously³¹^,³². This provides the opportunity for us to probe the SFG vibrational signal from only one interface. Here, the PHEMA film on the CaF₂ prism was taken as an example⁹.
As shown in Figure 3, employ the right-angle prism geometry to detect the SFG signals generated from the bottom PHEMA film. The SFG output intensity in the reflected mode is expressed as
(1)
where denotes the effective second-order nonlinear susceptibility tensor.
consists of three parts, namely, the prism/polymer interface, the polymer/bottom medium interface (bottom medium includes gas, liquid or solid.) and the nonresonant background, as shown in the following equation.
(2)
Here the bottom medium could be air, water or something else. F represents the corresponding Fresnel coefficient responsible for the local field correction.
Apply a thin-film model to calculate the Fresnel coefficients in this case. Here only brief calculation procedures are presented.
1. For the prism/polymer interface, use
  (3)
  (4)
  (5)
  The meaning of each parameter shown is presented below.
  1. ω_i denotes the beam frequency.
  2. t_p and t_s denote the overall transmission coefficients and can be expressed as
    (6)
    (7)
  3. t_p12 and t_s12 denote the linear transmission coefficients of the light beam at the prism/polymer interface.
  4. r_p23 and r_s23 denote the linear reflection coefficients of the light beam at the polymer/medium interface.
  5. α represents the phase difference between a reflective beam and its secondary reflective beam after it propagates across the polymer thin film and then reflects back, which can be expressed as
    (8)
  6. λ represents the wavelength of the light beam and d is the polymer film thickness.
  7. Φ₁ and Φ₂ represent the incident angles at the prism/polymer interface and the polymer/medium interface respectively.
  8. n₁ and n₂ represent the refractive indices of the prism and polymer film respectively.
  9. n₁₂ represents the refractive indices of the polymer interfacial layers for the prism/polymer.
2. For the polymer/medium interface, use
  (9)
  (10)
  (11)
  1. Δ represents the phase difference of the light electrical fields at two interfaces.
  2. Because the pulse width for our input beams is ~20 ps, the error from the time delay associated with the dispersion effect can be neglected.
  3. The expression of such phase difference for the output SFG, the input visible and the input infrared beams can be separately written as
    (12)
    (13)
    (14)
From the above discussion, for the prism-polymer film-medium (1-2-3) system, express the total Fresnel coefficients for the prism/polymer and polymer/medium interfaces as the following equations, for ssp and ppp polarization combinations. Of course, both interfaces are considered azimuthally isotropic.
1. For the prism/polymer interface, the expressions of the total Fresnel coefficients for both ssp and ppp polarization combinations are presented as follows.
  1. For ssp, the equation is
    (15)
  2. And for ppp, the equation is
    (16)
    (17)
    (18)
    (19)
  3. t₁₀ and t₀₁ denote the linear transmission coefficients at the air/prism and prism/air interfaces respectively.
2. For the polymer/medium interface, the expressions of the total Fresnel coefficients for both ssp and ppp polarization combinations are described as follows.
  1. For ssp, the equation is
    (20)
  2. For ppp, the equations are
    (21)
    (22)
    (23)
    (24)
After calculating the Fresnel coefficients using the sandwiched model, plot them as a function of the film thickness, as shown in Figure 4.
NOTE: In this case, there exists a thickness range for collecting the SFG signal from the CaF₂ prism/PHEMA interface with neglectable contribution from the other interface, which is around 150 nm. Similarly, a suitable thickness can be chosen for detection of the PHEMA/bottom medium interface with neglectable contribution from the CaF₂ prism/PHEMA interface.

3. Chiral SFG polarization combination

For the normal achiral interface, commonly, use C_∞v symmetry in terms of ensemble average³³^,³⁴. With operation of inversion symmetry, the nonzero second-order nonlinear susceptibility tensor components can be deduced, which are c_xxz, c_xzx, c_zxx, c_yyz, c_yzy, c_zyy and c_zzz (the existing terms can be further reduced if an isotropic interface is assumed, which means x and y are the same). However, for the chiral interface, situation will be different. The chiral interface possesses the C∞ symmetry, only the rotation symmetry operation is allowed. In this case, besides the normal achiral terms, more second-order nonlinear susceptibilities will be nonzero, which can be termed as the chiral terms, namely, c_zyx, c_zxy and c_yzx under the consideration of non-electronic resonance. Therefore, by using psp, pps and spp polarization combinations, chiral SFG spectra can be collected³³^,³⁴.

4. Sample preparation

Preparation of PHEMA film
1. Dissolve PHEMA powder (see Table of Materials) in anhydrous ethanol to prepare the solution with 2 wt% and 4 wt% respectively.
2. Before deposition of the PHEMA films, soak the CaF₂ right-angle prisms in the toluene solvent firstly and then wash them with ethanol and ultrapure water (18.2 MΩ·cm).
3. Afterwards, expose the substrates (CaF₂ right-angle prisms) to oxygen plasma to remove possible organic contaminants by plasma cleaner (see Table of Materials).
  1. First turn on the plasma cleaner and put the substrates in it.
  2. Then turn on the vacuum pump to vacuumize the cleaner. Input the oxygen in it.
  3. Finally set 4 minutes for cleaning. After that, preserve the clean substrates for the sequential PHEMA film preparation.
  4. Then prepare the PHEMA films on the CaF₂ prisms by a spin-coater (see Table of Materials). Adjust the film thicknesses by the solution concentration and spin speed.
    1. Immobilize the CaF₂ prism on the sucking disc of spin-coater.
    2. Drop one drop of the PHEMA solution prepared before onto the clean substrates at 1,500 rpm for 1 min (film thickness 2 wt% for 100 nm and 4 wt% for 200 nm).
  5. Anneal all the prepared PHEMA films in a vacuum oven at 80 °C overnight.
Preparation of silk fibroin (SF)
NOTE: The protocol suggested by Kaplan et al.³⁵ was adopted.
1. Place 7.5 g of silk cocoons of B. mori in the boiling sodium carbonate (Na₂CO₃, 0.02 M) aqueous solution (3 L) for 30 min. Remove the fibrous SF to a clean container.
2. Wash the obtained fibrous SF with deionized water for three times under stirring in order to remove the sericin molecules and leave only the SF molecules in the fibrous sample.
3. Dry the fibrous SF sample in a vacuum oven at 60 °C overnight.
4. Afterwards, dissolve the degummed fibrous SF sample in a lithium bromide (LiBr, 9.3 M) aqueous solution (1 g of SF was solved in ~4 mL of LiBr solution.) and incubate it at 60 °C for 2 h under stirring.
5. Dialyze the SF solution against deionized water (3,500 Da dialysis bags) for 3 days to remove the dissolved LiBr. Change new deionized water three times every day. Finally store the processed SF solution at 4 °C for later SFG experiments.
Preparation of short-chain oligonucleotide duplex
1. Order the single-stranded oligonucleotide sample with its 3’-end modified by cholesterol-triethylene glycol (Chol-TEG) (5’-GCTTCCGAAGGTCGA-3’) from a commercial corporation (see Table of Materials) as well as the complementary one. For each single strand, dissolve 10 nmol of the sample powder in 0.5 ml ultrapure water. Then mix them together to form the duplex oligonucleotide solution (10 nmol/mL).
2. Mix 2 mg of 1,2-Dipalmitoyl-sn-glycero-3-phosphocholine (DPPC) and 2 mg of deuterated DPPC (d-DPPC) and dissolve them in 1 mL of chloroform to prepare the lipid solution.
3. Preparation of DPPC & d-DPPC monolayer by a Langmuir−Blodgett (LB) trough
  1. Attach the right-angle CaF₂ prism to a homemade sample holder with one prism face perpendicularly dipped into the aqueous environment of the LB trough.
  2. Afterwards, inject the mixed lipid solution prepared before onto the water surface until the surface pressure reached a certain value below 34 mN·m⁻¹.
  3. After the surface pressure levels off, use two Teflon barriers to compress the lipid monolayer at a ratio of 5 mm/min until a surface pressure of 34 mN·m⁻¹ was reached.
  4. Lift the prism with a lipid monolayer out of the water at a rate of 1 mm/min vertically.
4. Preparation of the other lipid monolayer
  1. To facilitate the assembly of the duplex oligonucleotide and the lipid molecules via the hydrophobic interaction (cholesterol and a lipid alkyl chain), mix the duplex oligonucleotide solution with the lipid solution in a molar ratio of 1:100 (oligonucleotide to lipid).
  2. Inject the mixed lipid and duplex oligonucleotide solution onto the water surface in a homemade Teflon container until a surface pressure of 34 mN·m⁻¹ was reached.
5. Finally, put the lipid monolayer at the bottom of the prism in contact with the lipid monolayer with inserted duplex oligonucleotides on the water surface to form the final sample for the SFG measurement.
Lorentz equation
1. Use the Lorentz equation to fit the SFG spectra to extract the vibrational information for a specific vibrational mode.
  (25)
  where represents the intensity of the qth vibrational mode, represents the resonant frequency, denotes the half width at half maximum (HWHM) and represents the scanning frequency of the incident IR beam.

Representative Results

In the Fresnel coefficient part of Protocol Section, we have shown that, theoretically, it is feasible to selectively detect only one single interface at one time. Here, experimentally, we confirmed that this methodology is basically correct, as shown in Figure 5 and Figure 6.

Figure 5 shows the buried interfacial PHEMA structure after water intrusion with a ~150 nm PHEMA hydrogel film and Figure 6 shows the surface structure in water with a ~430 nm PHEMA hydrogel film. Panels A and B correspond to the CH and CO ranges respectively for both figures. At the buried interface, all the observed vibrational peaks are sharp and clear. The reason is that the CaF₂ substrate is smooth and cannot be penetrated by PHEMA molecules, leading to a sharp CaF₂/PHEMA interface. However, at the surface, because water molecules can interact with PHEMA and diffuse into the bulk, the PHEMA/water interface would be not as sharp as the buried one. Therefore, different spectral profiles are observed for these two interfaces.

Figure 1. Schematic show of the SFG process (left panel) with the energy transition diagram (right panel). Please click here to view a larger version of this figure.

Figure 2. The SFG system in the lab. Please click here to view a larger version of this figure.

Figure 3. Schematic shows the light propagation path in prism for SFG experiment. The numbers 0, 1, 2 and 3 represent the air, prism, PHEMA and bottom medium (the bottom medium can be air, solid or liquid.), respectively. Reproduced from Li, X.; Li, B.; Zhang, X.; Li, C.; Guo, Z.; Zhou, D.; Lu, X. Macromolecules 2016, 49, 3116−3125 (ref 9). Copyright 2016 American Chemical Society. This figure has been modified from [9]. Please click here to view a larger version of this figure.

Figure 4. Calculated Fresnel coefficients as a function of the film thickness for the prism geometry in water for ssp and ppp polarization combinations. Panels A1 세스 C1 correspond to the CH range and Panels A2 세스 C2 correspond to the CO range. Reproduced from Li, X.; Li, B.; Zhang, X.; Li, C.; Guo, Z.; Zhou, D.; Lu, X. Macromolecules 2016, 49, 3116−3125 (ref 9). Copyright 2016 American Chemical Society. This figure has been modified from [9].

Figure 5. ssp and ppp spectra of the CaF₂/PHEMA interface after water exposure. A: CH and OH range; B: CO range. The black curves are the fitted results by using Lorentz equation. The spectra have been offset for clarity. Reproduced from Li, X.; Li, B.; Zhang, X.; Li, C.; Guo, Z.; Zhou, D.; Lu, X. Macromolecules 2016, 49, 3116−3125 (ref 9). Copyright 2016 American Chemical Society. This figure has been modified from [9].

Figure 6. ssp and ppp spectra of the PHEMA surface on CaF₂ prism. A: CH and OH range; B: CO range. The sample was placed into contact with water. The black curves are the fitted results by using Lorentz equation. The spectra have been offset for clarity. Reproduced from Li, X.; Li, B.; Zhang, X.; Li, C.; Guo, Z.; Zhou, D.; Lu, X. Macromolecules 2016, 49, 3116−3125 (ref 9). Copyright 2016 American Chemical Society. This figure has been modified from [9].

Figure 7. Normalized chiral (psp) SFG spectra in the amide I (Panel A) and N-H (Panel B) ranges for the PS/SF solution (90 mg/mL) interface before and after adding methanol. The dots are experimental data and the solid lines are the fitted curves. Spectra have been offset for clarity. Reproduced from Li, X.; Deng, G.; Ma, L.; Lu, X.; Langmuir 2018, 34, 9453−9459 (ref 16). Copyright 2018 American Chemical Society. This figure has been modified from [16].

Figure 8. Normalized chiral (psp) SFG spectra in the amide I (Panel A) and N-H (Panel B) ranges for the PS/SF solution (1 mg/mL) interface before and after adding methanol. The dots are experimental data and the solid lines are the fitted curves (blue). Spectra have been offset for clarity. Reproduced from Li, X.; Deng, G.; Ma, L.; Lu, X.; Langmuir 2018, 34, 9453−9459 (ref 16). Copyright 2018 American Chemical Society. This figure has been modified from [16].

Figure 9. Achiral (ssp, A) and chiral (spp, B) SFG spectra for the duplex oligonucleotide-anchored lipid bilayer in contact with the Ca²⁺ solutions with different concentrations (from 0.6 mM to 6 mM). The data points were approximately fitted by using the Lorentz equation. The change of the integrated area for the water vibrational signals as a function of the Ca²⁺ concentration was presented (ssp, C; spp, D). All the spectra have been normalized and offset for clarity. Reproduced from Li, X.; Ma, L.; Lu, X.; Langmuir 2018, 34, 14774−14779 (ref 21). Copyright 2018 American Chemical Society. This figure has been modified from [21].

Discussion

To investigate the structural information from a molecular level, SFG has its inherent advantages (i.e., monolayer or sub-monolayer sensitivity and interfacial selectivity), which can be applied to study various interfaces, such as the solid/solid, solid/liquid, solid/gas, liquid/gas, liquid/liquid interfaces. Although the equipment maintenance and the optical alignment are still time-consuming, the payoff is significant in that the detailed molecular-level information at the surfaces and interfaces can be obtained.

Probing Poly(2-hydroxyethyl methacrylate) Surface and Buried interface in Solution: As we demonstrated above, the light field coefficients can be adjusted. We can confirm this experimentally. At the buried interface with the substrate, because the CaF₂ substrate surface is smooth and cannot be penetrated by PHEMA molecules, this interface is a sharp one. However, at the surface with water, water molecules can interact with PHEMA molecules and diffuse into the bulk. Hence this interface is blurry, and not as sharp as the buried one. Therefore, different SFG spectral profiles would be observed for these two interfaces. Our experimental SFG data did prove this, indicating the capability to selectively probe the buried interface with the substrate or the surface in solution.

Interchain Interaction or Confinement effect on Formation of Silk Fibroin Secondary Structures: A key factor is the critical overlapping concentration (C*). For SF, C* is ~1.8 mg/mL. Experimentally, for the SF solution of ~90 mg/mL (above C*), no chiral (psp) SFG vibrational signals were detected at the SF solution/PS interface unless an inducing agent-methanol was added, as shown in Figure 7. But, for the SF solution of ~1 mg/mL (below C*), chiral (psp) SFG vibrational signals can be directly detected without adding methanol, as shown in Figure 8, which indicates that the ordered secondary structures have already been formed at the SF solution/PS interface. Since C* is a threshold concentration for the chain-chain overlap, the chain-chain interaction or the spatial confinement has to be taken as a regulating factor here for the formation of SF secondary structures at the interface.

Water Molecular Structures Surrounding Short-chain Oligonucleotide Duplex: For a short-chain oligonucleotide duplex in the water solution, chiral water SFG vibrational signals correspond to the hydration layer of the chiral spine in the minor groove. Achiral water SFG vibrational signals mostly correspond to the water layer surrounding the oligonucleotide duplex chain and the bilayer (the chiral spine of the water layer also contributes)³³. In a Ca²⁺ concentration range from 0.6 to 6 mM, as shown in Figure 9, we found, there was no obvious change for the chiral water vibrational signals in terms of the Ca²⁺ concentration. However, the achiral water vibrational signals were strongly affected when the Ca²⁺ concentration was changed. This indicates that the chiral spine of the water layer closely binding to the oligonucleotide duplex may protect the oligonucleotide from the Ca²⁺ ions, in the normal biological condition.

Disclosures

The authors have nothing to disclose.

Acknowledgements

This study was supported by the State Key Development Program for Basic Research of China (2017YFA0700500) and the National Natural Science Foundation of China (21574020). The Fundamental Research Funds for the Central Universities, a project funded by the Priority Academic Program Development of Jiangsu Higher Education Institutions (PAPD) and the National Demonstration Center for Experimental Biomedical Engineering Education (Southeast University) were also greatly appreciated.

Materials

1,2-dipalmitoyl-sn-glycero-3-phosphocholine (DPPC)	Avanti Polar Lipids, Inc.	850355P-1g
Anhydrous ethanol	Sinopharm Chemical Reagent Co., Ltd	100092680	≥99.7%
CaF2 prism	Chengdu YaSi Optoelectronics Co., Ltd.
Calcium chloride anhydrous	Sinopharm Chemical Reagent Co., Ltd	10005817	≥96.0%
deuterated DPPC (d-DPPC)	Avanti Polar Lipids, Inc.	860345P-100mg
Electromagnetic oven	Zhejiang Supor Co., Ltd	C21-SDHCB37
Langmuir-Blodgett (LB) trough	KSV NIMA Co., Ltd.	KN 2003
Lithium bromide anhydrous	Sinopharm Chemical Reagent Co., Ltd	20056926
Milli-Q synthesis system	Millipore		Ultrapure water
Plasma cleaner	Chengdu Mingheng Science&Technology Co., Ltd	PDC-MG	Oxygen plasma cleaning
Poly(2-hydroxyethyl methacrylate) (PHEMA)	Sigma-Aldrich Co., LLC.	192066 MSDS	Mw = 300 000
Polystyrene	Sigma-Aldrich Co., LLC.	330345 MSDS	Mw = 48 kDa and Mn = 47 kDa
Silk cocoons			From Bombyx mori
Single complementary strand of oligonucleotide	Nanjing Genscript Biotechnology Co., Ltd.	H03596	5'-CGAAGGCTTCCAGCT-3'
Single strand of oligonucleotide	Nanjing Genscript Biotechnology Co., Ltd.	H04936	3¢-end modified by cholesterol-triethylene glycol(Chol-TEG) (5¢-GCTTCCGAAGGTCGA-3¢)
Sodium carbonate anhydrous	Sinopharm Chemical Reagent Co., Ltd	10019260	≥99.8%
Spin-coater	Institute of Microelectronics of the Chinese Academy of Sciences	KW-4A	For the prepartion of ploymer films
Step profiler	Veeco	DEKTAK 150	For the measurement of film thickness
Sum frequency generation (SFG) vibrational spectroscopy system	EKSPLA		A commercial picosecond SFG system

References

Shen, Y. R. Optical Second Harmonic Generation at Interfaces. Annual Review of Physical Chemistry. 40, 327-350 (1989).
Shen, Y. R. Surface properties probed by second-harmonic and sum-frequency generation. Nature. 337, 519-525 (1989).
Lu, X., et al. Studying Polymer Surfaces and Interfaces with Sum Frequency Generation Vibrational Spectroscopy. Analytical Chemistry. 89 (1), 466-489 (2017).
Chen, X., Clarke, M. L., Wang, J., Chen, Z. Sum Frequency Generation Vibrational Spectroscopy Studies on Molecular Conformation and Orientation of Biological Molecules at Interfaces. International Journal of Modern Physics B. 19 (4), 691-713 (2005).
Eisenthal, K. B. Liquid Interfaces Probed by Second-Harmonic and Sum-Frequency Spectroscopy. Chemical Reviews. 96 (4), 1343-1360 (1996).
Richmond, G. L. Molcular Bonding and Interactions at Aqueous Surfaces as Probed by Vibrational Sum Frequency Spectroscopy. Chemical Reviews. 102 (8), 2693-2724 (2002).
Wang, H., Gan, W., Lu, R., Rao, Y., Wu, B. Quantitative spectral and orientational analysis in surface sum frequency generation vibrational spectroscopy(SFG-VS). International Reviews in Physical Chemistry. 24 (2), 191-256 (2007).
Shultz, M. J., Schnitzer, C., Simonelli, D., Baldelli, S. Sum frequency generation spectroscopy of the aqueous interface: Ionic and soluble molecular solutions. International Reviews in Physical Chemistry. 19 (1), 123-153 (2010).
Li, X., et al. Detecting Surface Hydration of Poly(2-hydroxyethyl methacrylate) in Solution in situ. Macromolecules. 49, 3116-3125 (2016).
Li, X., Lu, X. Evolution of Irreversibly Absorbed Layer Promotes Dewetting of Polystyrene Film on Sapphire. Macromolecules. 51, 6653-6660 (2018).
Lu, X., Spanninga, S. A., Kristalyn, C. B., Chen, Z. Surface Orientation of Phenyl Groups in Poly(sodium 4-styrenesulfonate) and in Poly(sodium 4-styrenesulfonate): Poly(3,4-ethylenedioxythiophene) Mixture Examined by Sum Frequency Generation Vibrational Spectroscopy. Langmuir. 26 (17), 14231-14235 (2010).
Lu, X., Clarke, M. L., Li, D., Wang, X., Chen, Z. A Sum Frequency Generation Vibrational Study of the Interference Effect in Poly(n-butyl methacrylate) Thin Films Sandwiched between Silica and Water. Journal of Physical Chemistry C. 115, 13759-13767 (2011).
Lu, X., et al. Directly Probing Molecular Ordering at the Buried Polymer/Metal Interface 2: Using P-Polarized Input Beams. Macromolecules. 45, 6087-6094 (2012).
Lu, X., Myers, J. N., Chen, Z. Molecular Ordering of Phenyl Groups at the Buried Polystyrene/Metal Interface. Langmuir. 30, 9418-9422 (2014).
Li, B., Lu, X., Ma, Y., Han, X., Chen, Z. Method to Probe Glass Transition Temperatures of Polymer Thin Films. ACS Macro Letters. 4, 548-551 (2015).
Li, X., Deng, G., Ma, L., Lu, X. Interchain Overlap Affects Formation of Silk Fibroin Secondary Structure on Hydrophobic Polystyrene Surface Detected via Achiral/Chiral Sum Frequency Generation. Langmuir. 34, 9453-9459 (2018).
Kai, S., Li, X., Li, B., Han, X., Lu, X. Calcium-dependent hydrolysis of supported planar lipids was triggered by honey bee venom phospholipase A2 with the right orientation at the interface. Physical Chemistry Chemical Physics. 20, 63-67 (2018).
Wang, J., Buck, S., Chen, Z. Sum Frequency Generation Vibrational Spectroscopy Studies on Protein Adsorption. Journal of Physical Chemistry B. 106, 11666-11672 (2002).
Wang, J., et al. Detection of Amide I Signals of Interfacial Proteins in Situ Using SFG. Journal of American Chemical Society. 125, 9914-9915 (2003).
Nguyen, K. T., et al. Probing the Spontaneous Membrane Insertion of a Tall-Anchored Membrane Protein by Sum Frequency Generation Spectroscopy. Journal of American Chemistry Society. 132, 15112-15115 (2010).
Li, X., Ma, L., Lu, X. Calcium Ions Affect Water Molecular Structures Surrounding an Oligonucleotide Duplex as Revealed by Sum Frequency Generation Vibrational Spectroscopy. Langmuir. , (2018).
Sartenaer, Y., et al. Sum-frequency generation spectroscopy of DNA monolayers. Biosensors & Bioelectronics. 22, 2179-2183 (2007).
Asanuma, H., Noguchi, H., Uosaki, K., Yu, H. Metal Cation-induced Deformation of DNA Self-Assembled Monolayers on Silicon: Vibrational Sum Frequency Generation Spectroscopy. Journal of American Chemistry Society. 130, 8016-8022 (2008).
Howell, C., Schmidt, R., Kurz, V., Koelsch, P. Sum-frequency-generation spectroscopy of DNA films in air and aqueous environments. Biointerphases. 3 (3), FC47 (2008).
Walter, S. R., Geiger, F. M. DNA on Stage: Showcasing Oligonucleotides at Surfaces and Interfaces with Second Harmonic and Vibrational Sum Frequency Generation. Journal of Physical Chemistry Letters. 1, 9-15 (2010).
Li, Z., Weeraman, C., Azam, M. S., Osman, E., Gibbs-Davis, J. The thermal reorganization of DNA immobilized at the silica/buffer interface: a vibrational sum frequency generation investigation. Physical Chemistry Chemical Physics. 17, 12452-12457 (2015).
Lambert, A. G., Neivandt, D. J., Briggs, A. M., Usadi, E. W., Davies, P. B. Interference Effects in Sum Frequency Spectra from Monolayers on Composite Dielectric/Metal Substrates. Journal of Physical Chemistry B. 106, 5461-5469 (2002).
Tong, Y., et al. Interference effects in the sum frequency generation spectra of thin organic films. I. Theoretical modeling and simulation. Journal of Chemical Physics. 133, 034704 (2010).
McGall, S. J., Davies, P. B., Neivandt, D. J. Interference Effects in Sum Frequency Vibrational Spectra of Thin Polymer Films: An Experimental and Modeling Investigation. Journal of Physical Chemistry B. 108, 16030-16039 (2004).
Li, B., et al. Interfacial Fresnel Coefficients and Molecular Structures of Model Cell Membranes: From a Lipid Monolayer to a Lipid Bilayer. Journal of Physical Chemistry C. 118, 28631-28639 (2014).
Zhou, J., Anim-Danso, E., Zhang, Y., Zhou, Y., Dhinojwala, A. Interfacial Water at Polyurethane-Sapphire Interface. Langmuir. 31 (45), 12401-12407 (2015).
Gautam, K. S., et al. Molecular Structure of Polystyrene at Air/Polymer and Solid/Polymer Interfaces. Physical Review Letters. 85 (18), 3854-3857 (2000).
Yan, E. Y., Fu, L., Wang, Z., Liu, W. Biological Macromolecules at Interfaces Probed by Chiral Vibrational Sum Frequency Generation Spectroscopy. Chemical Reviews. 114, 8471-8498 (2014).
Belkin, M. A., Kulakov, T. A., Ernst, K. H., Yan, L., Shen, Y. R. Sum-Frequency Vibrational Spectroscopy on Chiral Liquids: A Novel Technique to Probe Molecular Chirality. Physical Review Letters. 85, 4474 (2000).
Rockwood, D. N., et al. Materials fabrication from Bombyx mori silk fibroin. Nature Protocols. 6, 1612-1631 (2011).

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Li, X., Ma, L., Lu, X. Interfacial Molecular-level Structures of Polymers and Biomacromolecules Revealed via Sum Frequency Generation Vibrational Spectroscopy. J. Vis. Exp. (150), e59380, doi:10.3791/59380 (2019).