Open Access

Raman and Luminescent Spectra of Sulfonated Zn Phthalocyanine Enhanced by Gold Nanoparticles

  • V. Kavelin1Email author,
  • O. Fesenko1,
  • H. Dubyna1,
  • C. Vidal2,
  • T. A. Klar2,
  • C. Hrelescu2 and
  • L. Dolgov3
Nanoscale Research Letters201712:197

Received: 13 January 2017

Accepted: 1 March 2017

Published: 16 March 2017


Sulfonated Zn phthalocyanine, as a prospective photosensitizer in the photodynamic therapy of tumors, is investigated by means of Raman, infrared, and fluorescence spectroscopies. Conventional and surface-enhanced spectra from this photosensitizer are obtained and compared. Gold nano-islands attached to silica cores (Au-SiO2) are proposed as nanostructures providing plasmonically enhanced signals. Pronounced enhancement of Raman and infrared spectral bands from sulfonated Zn phthalocyanine allows their more convenient assignment with vibrational modes of sulfonated Zn phthalocyanine. In comparison to Raman and IR, the fluorescence is less enhanced by Au-SiO2 particles.


Sulfonated Zn phthalocyanine (ZnPCSulf) Au-SiO2 nanoparticles Surface-enhanced Raman spectroscopy (SERS) Surface-enhanced infrared absorption (SEIRA)


The application of phthalocyanine compounds, in organic solar cells [1] or for cancer treatment [2, 3], renewed the research interest in such compounds, initially used only as dyes. Sulfonated metastable α-zinc phthalocyanine (α-ZnPc) and the stable β-zinc phthalocyanine (β-ZnPc) are not soluble in water [4]. Water solubility can be achieved by modifying the 3-sulfate-substituted ZnPc with L-cysteine radicals.

Noble metal nanoparticles can be used as optical nanoantennas for the enhancement of visible and infrared spectral signals for the detection of minute amount of analytes [5, 6]. Here, we propose specially prepared hybrid nanoparticles (Au-SiO2) for surface-enhanced Raman (SERS), surface-enhanced infrared (SEIRA), and visible range spectroscopies of phthalocyanine-based molecules. Our hybrid nanoparticles consist of dielectric silica nanospheres with diameters of 180 nm decorated with gold nano-islands with diameters in the range of 10–30 nm. In our case, gold nano-islands are randomly interconnected, in contrast to other reports where the dielectric cores were covered by a continuous shell [68]. Such incomplete, but dense, coverage of the dielectric cores with nano-islands is prone to enhance the Raman signals more than a complete homogeneous gold shell [9]. Here, we demonstrate that Au-SiO2 nanoparticles with an incomplete gold shell morphology can serve as SERS-SEIRA substrates for the detection of ZnPCSulf in the visible and infrared spectral range, while in earlier reports, only gold electrodes [10] or silver islands [11] were used for SERS detection of ZnPCSulf.

Both plasmonic enhancement and charge transfer from the nanoparticles to the ZnPCSulf molecules through the specific covalent thiol-gold (S-Au) bonds can be considered as possible enhancement mechanisms for surface-enhanced spectroscopy. Since in our case, the spectral ranges at which the SERS effect caused by charge transfer and plasmonic resonance are spectrally overlapped and are hardly separable; we associate the measured SERS enhancements of ZnPc signals with both mechanisms. Impact of chemical enhancement, namely possible charge transfer from the substrate to the analyte molecules, can be investigated separately on the examples of analytes deposited on graphene surface [12]. The SERS/SEIRA enhancements allow a better than for conventional spectroscopy assignment of observed spectral bands with molecular vibrations, rendering our Au-SiO2 nanoparticles as promising SERS-SEIRA substrates with satisfactory enhancement of broadband spectral signals.


Both 3-sulfate-substituted ZnPc and ZnPc with one substituent modified by L-cysteine radicals were produced by the NIOPIK company (Russia) with a purity of 92%. Here, only the main steps of synthesis are noted. Particularly, trisodium salt of zinc phthalocyanine was synthesized from trisulfonic acid by sulfonation of unsubstituted phthalocyanine with chlorosulfonic acid in inert high-boiling solvents (o-dichlorobenzene, trichlorobenzeze) [13]. The schematic representation of ZnPCSulf molecule and designation of standard connections are shown in Fig. 1. The replacement of one of the sulfate functional groups of the ZnPCSulf by L-cysteine was conducted according to ref. [14].
Fig. 1

Schematic representation of ZnPCSulf molecule and designation of standard connections. a ZnPCSulf molecule. b Isoindole radical. c Pyrrole group or macrocycle

Monodispersed 150–180 nm silica spheres were prepared by the Stöber method from tetraethyl orthosilicate as a dispersion in ethanol [15]. Gold seeds of 5–10 nm in diameter were prepared in water by reduction of chloroauric acid (HAuCl4) with tetrakis(hydroxymethyl)phosphonium chloride working also as a stabilizing agent. Silica nanoparticles were functionalized with (3-amino)propyltrimethoxysilane. When silica and gold nanoparticle dispersions are mixed, the resultant terminal amine groups on the silica surface act as attachment points for the small gold seeds [8]. After washing by centrifugation, the hybrid nanoparticles (Au-SiO2) were finally redispersed in water (~109 1/cm3) by ultrasonication.

A solution of 10 μg/ml of ZnPCSulf in water was used as reference. Then, 100 μl of this solution was mixed with 20 μl of Au-SiO2 NP dispersion (concentration of NPs ~109 1/ml). These tested and reference mixtures were used without additional modifications in fluorescence and light extinction measurements. The samples for Raman and infrared measurements were prepared in a similar way. Namely, equal amounts of 20 μl droplets from tested and reference mixtures were drop-casted on a glass (for Raman) and on BaF2 substrates (for infrared) and dried at room temperature. Line scans of the droplets from tested and reference mixtures were compared in terms of their Raman and infrared spectra.

The Raman spectra were obtained with an inVia micro-Raman spectrometer (Renishaw plc, Wotton-under-Edge, UK) at the HeNe laser excitation wavelength of 633 nm. IR spectra were measured by FTIR spectrometer (VERTEX, Bruker, Germany). Light extinction by the solutions was measured by the Cary 500 Scan UV-Vis-NIR Spectrometer. Luminescence of solutions was measured by FluoroLog-2 spectrofluorimeter (Instruments SA). All measurements were performed at room temperature.

Raman and IR experiments probing intrinsic fingerprint spectra of analytes were carried out in dry environment because they are often used in the format of drop casting and drying. In contrast, fluorescence enhancement assays need a detection step in aqueous environment, and hence, we measured fluorescence in aqueous solution [16].

Results and Discussion

Optical Properties of Au-SiO2 Nanoparticles

The hybrid Au-SiO2 nanoparticles consist of dielectric silica nanospheres with diameters of 180 nm decorated with gold nano-islands with diameters in the range of 10–30 nm. In Fig. 2, a scanning electron microscopy (SEM) image of representative Au-SiO2 nanoparticles is shown. The Au-SiO2 nanoparticles possess a corrugated surface caused by separated as well as partially connected gold nano-islands.
Fig. 2

Scanning electron microscopy of precipitated Au-SiO2 nanoparticles

Solutions of Au-SiO2 nanoparticles dispersed in water exhibit a blue-violet color (Fig. 3a).
Fig. 3

a Water dispersion of Au-SiO2 nanoparticles. b Optical density (OD) of an aqueous dispersion of Au-SiO2 nanoparticles in a cuvette with 10 mm of optical path length, corrected by the OD of a cuvette filled with water without nanoparticles

The extinction of the Au-SiO2 nanoparticles, as shown in Fig. 3b, can be explained by the Mie light scattering from the SiO2 particles together with a plasmon peak at 535 nm which is expected for gold nanoparticles with dimensions in the range of 10–30 nm [17]. The additional spectral shoulder at 611 and 665 nm is most probably caused by plasmonic coupling of neighboring gold nano-islands on the silica cores.

The combination of SEM imaging with subsequent dark field spectroscopy of the same single nanoparticles allowed us to measure the light-scattering spectrum from a selected individual Au-SiO2 nanoparticle (Fig. 4a) and to correlate its shape and size directly to its scattering spectrum (Fig. 4b). This particular example shows a broad maximum at 750 nm. The maximum at 750 nm can be attributed to the coupling of several plasmon resonances from the gold nano-islands attached to the silica core.
Fig. 4

a SEM image of a representative Au-SiO2 nanoparticle. b Scattering spectrum of the Au-SiO2 nanoparticle depicted in (a)

Extinction Spectra of ZnPCSulf Solutions With and Without Au-SiO2

The extinction spectrum of ZnPCSulf aqueous solutions with and without Au-SiO2 is shown in Fig. 5. The increased extinction between 350 and 450 can be attributed to the Soret band (B band) absorption. The two maxima at 634 and 665 nm can be attributed to the main absorption within the Q band of ZnPCSulf [18, 19].
Fig. 5

UV-VIS spectra of ZnPCSulf (black line) and ZnPCSulf with Au-SiO2 nanoparticles (red line)

The addition of Au-SiO2 causes the appearance of additional maximum at 533 nm associated with the plasmon resonances of the gold nano-islands. Further, the Mie light scattering from the silica cores causes an overall increase and reshaping of the extinction spectra of ZnPCSulf solutions with Au-SiO2 compared to the extinction spectra of pure ZnPCSulf solutions.

Luminescence of ZnPCSulf Solutions With and Without Au-SiO2

The luminescence spectra from ZnPCSulf solutions exhibit a main band at 675 nm and a shoulder at 750 nm. The spectral positions of these emission bands do not change for different excitation wavelengths, λ exc = 405 and 532 nm, Figs. 6a, b, respectively. The fluorescence is more pronounced for λ exc = 405 nm because of a higher absorption coefficient of ZnPCSulf at 405 nm (Soret band) than that at 532 nm. The fluorescence emission coincides with the electronic HOMO-LUMO (Q bands) transitions [20].
Fig. 6

Fluorescence spectra of ZnPCSulf solutions with and without Au-SiO2 nanoparticles: a for an excitation resonant to the Soret band of the ZnPCSulf (λ exc = 405 nm) and (b) for an excitation wavelength resonant to the dipolar plasmon mode of the gold nano-islands (λ exc = 532 nm)

When the ZnPCSulf solutions containing Au-SiO2 nanoparticles are excited within the Soret band of the ZnPCSulf (excitation wavelength at λ exc = 405 nm in Fig. 6a), the detected fluorescence intensity is more than 20% higher compared to the intensity of the ZnPCSulf solutions without Au-SiO2 nanoparticles.

The distance between the metal nanoparticles and fluorophores and the orientation of the molecular dipoles determine if the fluorescence is enhanced or quenched [19]. If the position of the fluorophores is at a distance smaller than 5 nm from the metal nanoparticle, the fluorescence may be quenched by energy transfer. In addition, quenching can be achieved by out-of-phase dipole coupling. Energy transfer acts on short range (10 nm and less); out-of-phase effects act on ranges up to 20 nm [21].

If, however, the molecular dipole and the image dipole act in phase, an enhancement of fluorescence can be expected at distances of tens of nanometers [22, 23]. At such distances, the quenching is less probable but the fluorophores are still situated in proximity of the nanoparticles. Additionally, locally enhanced electric fields lead to a higher excitation probability close to the metal nanoparticles. In total, if the fluorescent dipole has a proper orientation with respect to the nanoparticle surface, the excitation and the radiative rate of the fluorophores are increased. Even in these conditions, experimental observation of plasmon-coupled fluorescence is not easy for single particles.

Since in solution, the distance between ZnPCSulf molecules and Au-SiO2 nanoparticles depends on concentration and since the nanoparticles and fluorophore molecules move stochastically in solution, no accurate control of the distance between the ZnPCSulf molecules and Au-SiO2 nanoparticles was achieved. However, in both experiments, no quenching but fluorescence enhancement was observed (Table 1). The fact that excitation of the ZnPCSulf solutions with Au-SiO2 nanoparticles, resonant to the Soret band of the ZnPCSulf, leads to a more pronounced fluorescence enhancement (of 20%) with respect to the reference than the excitation resonant to the dipolar mode of the gold nano-islands can be carefully attributed to the higher Mie scattering of the SiO2 nanoparticles at 405 nm than that at 532 nm, which might cause a higher absorption probability. It seems that the local field enhancement occurring due to resonant excitation of the dipolar plasmon mode of the gold nano-islands does not lead to a substantial increase in the excitation probability of the ZnPCSulf molecules. More pronounced fluorescence enhancements might be obtained from aggregates of several metal nanoparticles, where a proper spacing of the fluorophores to the metal is achieved and where several strong hotspots occur in the gaps between the nanoparticles [24].
Table 1

Luminescence of ZnPCSulf with and without Au-SiO2 nanoparticles for different excitation wavelengths

Excitation wavelength

Emission wavelength, nm


Relative enhancement %


ZnPCSulf with Au-SiO2

405 nm (Soret band)









532 nm (resonant to the gold nano-island plasmons)









IR Spectra of ZnPCSulf Samples

The IR spectra of ZnPCSulf samples with and without Au-SiO2 as well as the band assignments of the detected spectral bands with the bond vibrations in the Zn phthalocyanine molecules are shown in Fig. 7. Surface-enhanced infrared absorption (SEIRA) for ZnPCSulf containing Au-SiO2 was detected. The infrared bands of ZnPCSulf were enhanced up to five times by the Au-SiO2 depending on the type of molecular group. Commonly in SEIRA, this enhancement is provided by electromagnetic interactions due to the surface plasmon resonance in the metal nanostructures and by changes in molecular dipole moments when the molecules are adsorbed on metal nanostructures [25]. In our case, the dominant role in the enhancement could be played by the molecular mechanism due to the fact that the vibronic (IR spectrum) of ZnPCSulf overlaps only partially with the spectral tail of the plasmon resonances of the Au-SiO2 nanoparticles and hence, the electromagnetic enhancement is not high.
Fig. 7

IR spectra of ZnPCSulf, ZnPCSulf with Au-SiO2, and pure Au-SiO2

The IR spectra of ZnPCSulf exhibit a band at 1614 cm−1, which is characteristic for compounds containing the benzene rings and connected with C-C stretching vibrations (Fig. 7) [26]. The shift of this band to lower frequencies by 5 cm−1 can be caused by deuteration.

The bands at frequencies 1415 and 1348 cm−1 are related to isoindole stretching and coupling of pyrrole and isoindole stretching vibrations, respectively [27]. The frequencies of in-plane vibrations with large contributions of the C-C-H mode fall within the 1000–1300 cm−1 range. Two bands at frequencies 729 and 816 cm−1 relate to in-plane skeletal vibrations (Table 2) [26].
Table 2

Assignment of the IR spectral bands with molecular vibrations in ZnPCSulf

ZnPCSulf, v (cm−1)

ZnPCSulf with AuSiO2, v (cm−1)




C-C stretching vibrations of pyrrole ring, O-H, N-H



C-C stretching vibrations of the benzene rings, C = C



Isoindole stretching coupling of pyrrole, C-H






C-H deformations of the isoindole ring, plane skeletal vibrations



Plane skeletal vibrations

Raman Spectra of ZnPCSulf Samples

Raman spectra of ZnPCSulf are shown in Fig. 8a. Most of the ZnPCSulf Raman bands correspond to deformations and stretching vibrations of chemical bonds of carbon atom with hydrogen, nitrogen, and characteristic vibrations of nitrogen-zinc bonds (Fig. 8). It is known that the most intense Raman peaks appeared from the non-polar functional groups, due to stronger change of dipole moments and their polarizability [28]. Therefore, the oscillations of double and triple carbon bonds and aromatic groups of symmetric vibrations are significantly enhanced in comparison with such as C-H; O-H; C = O; S-H [29].
Fig. 8

Raman spectra of ZnPCSulf (a), ZnPCSulf mixed with Au-SiO2 nanoparticles, and pure Au-SiO2 nanoparticles (b)

For the range of low frequencies (~1000 to 100 cm−1), it is typical to observe intra-molecular and crystal vibrations [28]. Since the ZnPCSulf molecule does not have hydrogen atoms that directly connect with the ring surrounding of the central metal atom, the stretching vibrations of C-H bonds have a much higher frequency compared to the frequency of the macrocycle fluctuations. The C-H vibrations should appear around 3000 cm−1 and have a low intensity [30].

Symmetric valence and deformation vibrations of Zn-Na bonds [31] are connected with the peak at 747 cm−1 (Fig. 8a). The most intense peak located at 1521 cm−1 (Fig. 8a) can be attributed to vibrations of completely symmetrical bonds, such as symmetric valence Ca = Cв vibrations in benzene rings and Ca = Nв vibrations in pyrrole structures [32]. In the spectral range below 1000 cm−1, vibrational motion of the pyrrole groups dominates in the spectra.

Mixing of ZnPCSulf with Au-SiO2 nanoparticles resulted in the significant enhancement of its Raman signal (Fig. 8b).

As a result of ZnPCSulf interaction with gold, the peaks at 1521 and 1337 cm−1 are shifted and significantly increased. The increase of intensity can be attributed to pyrrole molecules chemically bonded with gold [10]. The peak at 952 cm−1 corresponds to out-of-plane vibrations of C-H bonds. Similar vibrations occur in the bis- and three-phthalocyanine structures.

The changes in intensity and position of Raman spectral bands caused by addition of Au-SiO2 nanoparticles to the ZnPCSulf are depicted in Table 3.
Table 3

Assignment of the Raman spectral bands with molecular vibrations in the ZnPCSulf

ZnPCSulf, cm−1

ZnPCSulfwith Au-SiO2, cm−1



IZnPCSulf with Au-SiO2 /IZnPCSulf



Zn-N, pyrrole out-of-plane, Na-Ca-Nb




radial Au-S stretching modes



Au-S vibration



Au-S vibration




Macrocycle bending of pyrrole





Out-of-plane C-H, C-N-C, deformations of the isoindole ring





C-C-C benzene, C-S





Ca, Na, out-of-plane, C-S





Ca-N-Ca, C-C-N, Zn-Na, antisymmetric deformation of the macrocycle





C-H out-of-plane, C-C-C pyrrole, and vibrations of benzene groups





Ca-Cб, C-H benzene, Cб-Cб, stretching vibrations of pyrrole groups





Ca-N, N-Ca-Na, Ca-N-Ca





H-Ca-Cb, Ca = Nb, Ca-Cb,





Ca = Cb





Ca = Cb, Ca = Nb, and stretching vibration in the pyrrole group are totally symmetric vibration



As one can see from Table 3, there are changes in the position of ZnPCSulf spectral bands caused by Au-SiO2 nanoparticles. These changes are connected with fluctuations of bonds in pyrrole ring and can be represented as 720 cm−1 → 707 cm−1, 1149 cm−1 → 1136 cm−1, 1272 cm−1 → 1262 cm−1, and 1337 cm−1 → 1313 cm−1. Particularly, the peaks at 1337 and 1521 cm−1 correspond to the valence and deformation vibrations of pyrrole rings. Reduction-oxidation processes in ZnPCSulf can be located at the ligand and at the metal center of ZnPCSulf. The ZnPCSulf ring can undergo successive one-electron reduction and one-electron oxidation to yield the anion and cation radicals.

The thiol group (H-S) reacts with Au nanoparticles and forms very stable covalent metal-sulfur bonds [33]. Usually, the characteristic peak for the S-H group of ZnPCSulf is observed at 2546 cm−1, but in case of ZnPCSulf mixed with Au-SiO2 nanoparticles, no such specific band was detected. The absence of the S-H peak indicates that there was a chemical interaction with the formation of S-Au bond [34]. As an important feature in the spectra of ZnPCSulf with Au-SiO2, multiple Au-S stretching modes were observed at about 250 cm−1 (black spectra in Figs. 8b). Nanostructures, such as Au-SiO2 nanoparticles, should give rise to multiple Au-S stretching modes at different frequencies due to the different nature of the Au-S bonds involved (Au-S within the staple structure, where ZnPCSulf can be confined between different gold islands or different Au-SiO2 nanoparticles and Au-S involving a core gold atom) [35].

The enhancement factor for spectral signals of some molecular groups of ZnPc reaches up 65 times for SERS and 5–6 times in SEIRA effect. This can be deduced by the fact that a molecular mechanism is only present in IR spectroscopy because SEIRA experiments were carried out on the tail of the plasmon resonance. However, chemical and electromagnetic mechanisms of enhancement play a role in Raman spectroscopy because a laser with a wavelength of 633 nm is used, which almost coincides with one of the plasmonic frequencies which excited in the gold islands (see Fig. 3b). The appearance of Au-S bands at 275 and 289 cm−1 points on a chemical bond between Au and ZnPc.


Conventional and surface-enhanced spectra from 3-sulfate-substituted zinc phthalocyanine having the L-cysteine radicals are investigated and compared. Plasmonic gold nano-islands attached to silica cores showed potential as universal SEIRA-SERS broadband substrates. These nanostructures are suitable both for a moderate enhancement of fluorescence and for essential enhancements of Raman and IR signals of sulfonated Zn phthalocyanine. The enhancement of observed Raman signal is mainly caused by plasmonic mechanism of SERS. The chemical contribution to enhancement is possibly caused by charge transfer through the Au-S bonds, according to the Raman spectral data. The SERS spectral bands show significant enhancement and some shifts of spectral peaks when compared with ordinary Raman scattering spectra. At the same time, the plasmonic influence on the fluorescence of sulfonated Zn phthalocyanine appeared moderate, which can be attributed to the random spacing between the ZnPC molecules and Au-SiO2 nanoparticles. The weaker, as compared to the Raman, enhancement can also be explained by the fact that in case of fluorescence, we measured ensembles of nanoparticles in solution while, in case of Raman and IR measurements, the signals were obtained from dense layers of closely packed particles.

Au-SiO2 nanoparticles are promising candidates as SERS-SEIRA substrates for broadband spectroscopic material identification of very thin films and monolayers of biological molecules. The presented results can be useful for the elaboration of SEIRA and SERS sensors for detection of small amounts of chemical reagents and their spectral characterization.



Silica core-gold shell nanoparticle


Highest occupied molecular orbital


Infrared spectroscopy


Lowest unoccupied molecular orbital


Surface-enhanced infrared absorption


Scanning electron microscope


Surface-enhanced Raman spectroscopy


Zn phthalocyanine


Sulfonated Zn phthalocyanine



This work was supported by the Marie Curie ILSES project no. 612620 and NATO SPS project NUKR.SFPP984702. Authors also acknowledge Dr. A. Ryabova from the A.M. Prokhorov General Physics Institute, RAS, Moscow, for the fruitful discussions.

Authors’ Contributions

OF conceived the work, measured and analyzed the Raman spectra and took part in writing the manuscript. HD took part in the assignment of the Raman modes. VK measured and analyzed the IR spectra and took part in writing the manuscript. TK discussed the results. CV measured the UV-VIS spectra and luminescence and took part in writing the manuscript. CH took part in the analyses of the experimental data and writing of the article. LD synthesized the Au-SiO2 nanoparticles and actively participated in the discussion and description of the revealed plasmonic influence on the light absorption, fluorescence, and Raman scattering. All authors read and approved the final manuscript.

Competing Interest

The authors declare that they have no competing interests.

Publisher’s Note

Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.

Open AccessThis article is distributed under the terms of the Creative Commons Attribution 4.0 International License (, which permits unrestricted use, distribution, and reproduction in any medium, provided you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made.

Authors’ Affiliations

Institute of Physics of NAS of Ukraine
Institute of Applied Physics, Johannes Kepler University Linz
Institute of Physics, University of Tartu


  1. Walter M, Rudine A, Wamser C (2010) Porphyrins and phthalocyanines in solar photovoltaic cells. J Porphyrins Phthalocyanines 14:759–792View ArticleGoogle Scholar
  2. Swavey S, Tran M (2013) Porphyrin and phthalocyanine photosensitizers as PDT agents: a new modality for the treatment of melanoma. In: Davids LM (ed) Recent Advances in the Biology, Therapy and Management of Melanoma. INTECH Open Access Publisher, Rijeka, Croatia, pp 253–282Google Scholar
  3. Vasilchenko S, Volkova AI, Ryabova AV, Loschenov VB, Konov VI, Mamedov AA, Kuzmin SG, Lukyanets EA (2010) Application of aluminum phthalocyanine nanoparticles for fluorescent diagnostics in dentistry and skin autotransplantology. J Biophotonics 4:336–346View ArticleGoogle Scholar
  4. Kozlik M, Paulke S, Gruenewald M, Forker R, Fritz T (2012) Determination of the optical constants of α-and β-zinc (II)-phthalocyanine films. Org Electron 13:3291–3295View ArticleGoogle Scholar
  5. Tapan K, Rogach A (2012) Complex-shaped metal nanoparticles: bottom-up syntheses and applications. John Wiley & Sons, Weinheim, GermanyGoogle Scholar
  6. Khlebtsov N, Dykman L (2010) Handbook of photonics for biomedical science. CRC Press Boca Raton, FL, pp 37–82View ArticleGoogle Scholar
  7. Oldenburg J et al (1999) Nanoengineering of optical resonances. Chem Phys Lett 300:243–247View ArticleGoogle Scholar
  8. Pham T, Jackson JB, Halas NJ, Lee TR (2002) Preparation and characterization of gold nanoshells coated with self-assembled monolayers. Langmuir 18:4915–4920View ArticleGoogle Scholar
  9. Oldenburg SJ, Westcott SL, Averitt RD, Halas NJ (1999) Surface enhanced Raman scattering in the near infrared using metal nanoshell substrates. J Chem Phys 111:4729–4735View ArticleGoogle Scholar
  10. Palys BJ, Puppels GJ, Van den Ham D, Feil D (1992) Raman spectra of zinc phthalocyanine monolayers adsorbed on glassy carbon and gold electrodes by application of a confocal Raman microspectrometer. J Electroanal Chem 326:105–112View ArticleGoogle Scholar
  11. Jennings C, Aroca R, Hor AM, Loutfy RO (1984) Surface-enhanced Raman scattering from copper and zinc phthalocyanine complexes by silver and indium island films. Anal Chem 56:2033–2035View ArticleGoogle Scholar
  12. Fesenko O, Dovbeshko G, Dementjev A, Karpicz R, Kaplas T, Svirko Y (2015) Graphene-enhanced Raman spectroscopy of thymine adsorbed on single-layer graphene. Nanoscale Res Lett 10:163View ArticleGoogle Scholar
  13. Derkacheva V, Vazhnina V, Kokoreva V, Lukyanets E (2015) Method for producing sulphonated phthalocyanines., Patent of Russian Federation No2181736Google Scholar
  14. Dement’eva OV, Vinogradova MM, Luk’yanets EA, Solov’eva LI, Ogarev VA, Rudoy VM (2014) Zinc phthalocyanine-based water-soluble thiolated photosensitizer and its conjugates with gold nanoparticles: synthesis and spectral properties. Colloid J 76:539–545View ArticleGoogle Scholar
  15. Stöber W, Fink A, Bohn E (1968) Controlled growth of monodisperse silica spheres in the micron size range. J Colloid Interface Sci 26:62–69View ArticleGoogle Scholar
  16. Klar TA (2007) In: Kawata S, Shalaev V (eds) Advances in nano-optics and nano-photonics, vol 2. Elsevier, AmsterdamGoogle Scholar
  17. Kreibig U, Vollmer M (2013) Optical properties of metal clusters, vol 25. Springer Science & Business MediaGoogle Scholar
  18. Seoudi R, El-Bahy GS, El Sayed Z (2006) Ultraviolet and visible spectroscopic studies of phthalocyanine and its complexes thin films. Opt Mater 29:304–312View ArticleGoogle Scholar
  19. Mack J, Stillman MJ (1997) Assignment of the optical spectra of metal phthalocyanine anions. Inorg Chem 36:413–425View ArticleGoogle Scholar
  20. Ogunsipe A, Chen JY, Nyokong T (2004) Photophysical and photochemical studies of zinc (II) phthalocyanine derivatives—effects of substituents and solvents. New J Chem 28:822–827View ArticleGoogle Scholar
  21. Dulkeith E, Ringler M, Klar TA, Feldmann J, Munoz Javier A, Parak WJ (2005) Gold nanoparticles quench fluorescence by phase induced radiative rate suppression. Nano Lett 5:585–589View ArticleGoogle Scholar
  22. Anger P, Bharadwaj P, Novotny L (2006) Enhancement and quenching of single-molecule fluorescence. Phys Rev Lett 96:113002View ArticleGoogle Scholar
  23. Lakowicz JR (2001) Radiative decay engineering: biophysical and biomedical applications. Anal Biochem 298:1–24View ArticleGoogle Scholar
  24. Teixeira R, Paulo PM, Viana AS, Costa SM (2011) Plasmon-enhanced emission of a phthalocyanine in polyelectrolyte films induced by gold nanoparticles. J Phys Chem 115:24674–24680Google Scholar
  25. Kundu J, Le F, Nordlander P, Halas NJ (2008) Surface enhanced infrared absorption (SEIRA) spectroscopy on nanoshell aggregate substrates. Chem Phys Lett 452:115–119View ArticleGoogle Scholar
  26. Gladkov LL, Shkirman SF, Sushko NI, Konstantinova VK, Sokolov NA, Solovyov KN (2001) IR spectra of Zn phthalocyanine and Zn phthalocyanine-d 16 and their interpretation on the basis of normal coordinate analysis. Spectrosc Lett 34:709–719View ArticleGoogle Scholar
  27. Jiang J, Arnold DP, Yu H (1999) Infra-red spectra of phthalocyanine and naphthalocyanine in sandwich-type (na) phthalocyaninato and porphyrinato rare earth complexes. Polyhedron 18:2129–2139View ArticleGoogle Scholar
  28. Myronov V, Yankovskiy S. Handbook: Spectroscopy in organic chemistry, M.:Chemistry, 1985. 232 (in Russian)Google Scholar
  29. Basak S, Sen S, Roy P, Gómez-García CJ, Hughes DL, Butcher RJ, Mitra S (2010) Structural Variation and Magneto-Structural Correlation in Two New Dinuclear Bis (μ 2-Phenoxo)-Bridged Cu II Schiff-Base Complexes: Catalytic Potential for the Perox idative Oxidation of Cycloalkanes. Aust J Chem 63:479–489View ArticleGoogle Scholar
  30. Vandenabeele P (2013) Practical Raman spectroscopy: an introduction. John Wiley & Sons, Hoboken, NJView ArticleGoogle Scholar
  31. Palys BJ, Ham DM, Briels W, Feil D (1995) Resonance Raman spectra of phthalocyanine monolayers on different supports. A normal mode analysis of zinc phthalocyanine by means of the MNDO method. J Raman Spectrosc 26:63–76View ArticleGoogle Scholar
  32. Gladkov LL, Konstantinova VK, Ksenofontova NM, Sokolov NA, Solov'ev KN, Shkirman SF (2002) Resonant Raman Scattering Spectra of Zn‐Phthalocyanine and Zn‐Phthalocyanine‐d16. J Appl Spectrosc 69:47–57View ArticleGoogle Scholar
  33. Aryal S, Remant BKC, Dharmaraj N, Bhattarai N, Kim CH, Kim HY (2006) Spectroscopic identification of S< img border=. Spectrochim Acta A Mol Biomol Spectrosc 63:160–163View ArticleGoogle Scholar
  34. Gladkov LL, Gromak VV, Konstantinova VK (2007) Interpretation of resonance Raman spectra of Zn-phthalocyanine and Zn-phthalocyanine-d16 based on the density functional method. J Appl Spectrosc 74:328–332View ArticleGoogle Scholar
  35. Bürgi T (2015) Properties of the gold–sulphur interface: from self-assembled monolayers to clusters. Nanoscale 7:15553–15567View ArticleGoogle Scholar


© The Author(s). 2017