Research
Design and implementation of an experimental Raman
spectrometer
F.S. Chiwoa
F.J. Gonzáleza
*
aTerahertz Science and Technology National
Lab. Autonomous University of San Luis Potosí, Sierra Leona 550 Lomas 2nd
Sección San Luis Potosi, SLP, 78210 México.
Abstract
Non-invasive medical diagnosis has become popular due to the possibility of
detecting illnesses in vivo and in real time this technique, often referred to
as “optical biopsy” it comprises several optical techniques such as
thermography, diffuse reflectance spectroscopy, optical coherence tomography and
Raman spectroscopy among others. Particularly Raman spectroscopy is an optical
technique based on the inelastic scattering of light that can detect disease
markers, this technique has been successfully used to detect several types of
diseases, however the high price of a Raman spectrometer makes it difficult for
the medical community to adopt its use as a common diagnostic procedure. In this
work, an experimental Raman spectrometer was designed and fabricated from
low-cost readily available components. The system was characterized and the
Raman spectra obtained was compared to commercial systems. Results show that it
is possible to fabricate an experimental Raman system with the desired optical
configuration and with some improvements in the selected commercial components,
it could be useful for non-invasive medical diagnosis.
Keywords: Raman spectroscopy; electronic instrumentation; laser technology
PACS: 07.50.Ek; 07.57.Ty; 07.60.-j
1. Introduction
Raman Spectroscopy is a technique based on an optical phenomenon first reported by C.
V. Raman [1], in which a beam of light
inciding on a sample generates inelastic collisions between the photons of the
incident beam and the molecules of the sample, producing scattering with a
frequency-shift due to the gain or loss in energy by the inelastic collisions. These
frequency-shifts are known as Raman shifts and give detailed information about
molecules that are Raman active [2-5]. Every Raman active molecule has a
characteristic Raman spectrum which is unique to that molecule and can be considered
a fingerprint for that molecule. This technique has a wide range of applications in
different fields. For instance, in the case of medical diagnosis the technique has
several advantages over the traditional biopsy since it provides results in real
time, it makes sample preparation unnecessary and it is nondestructive [6]. Although a Raman spectrometer can be used
for medical diagnosis depending on its sensitivity, specificity and low cost [7,8],
currently these devices are not commonly used by the medical community mainly
because their extremely high prices and their size, which is too large to carry it
around a hospital. In this work, a methodology of design for an experimental Raman
spectrometer is proposed and then validated following an implementation with
commercial components
2. Methods
The design presented in this work is based on previously proposed designs [9,10],
that consists on a light source, a waveguide for excitation and detection, a
detector and a PC for data processing. The major opto-electronical components of the
proposed Raman spectrometer were from Ocean Optics: the calibration source, the
light source and the optic probes. Also, some optical-mechanical components used
were from Thorlabs: the light source and its driver, a notch filter to reject the
pump wavelength and two micro-positioners for fixing this optical filter. For the
data acquisition, the software Ocean Optics Spectra Suite was used and the data
processing was performed using the MatlabTM software (The MathWorks Inc., Natick,
Massachusetts, USA). The light source used was a single mode fiber pigtailed NIR
diode laser Thorlabs LP785SF-100 with a pump wavelength of 785 nm and optical power
regulable from 0-100 mW, its principle of operation is ruled by the Eq. (1) and for the optical-electrical
characterization of the diode laser, an optical power meter Newport was used.
P(I)=0.5I-40,if 80≤I≤310.0,if 0≤I≤80.
(1)
where I is the current measured and P is the optical power obtained. This principle of operation is shown in
the Fig. 1.
For the system waveguide, the optical fiber pigtailed to the diode laser was
connected via a matching sleeve to a multimode optical probe R200-7-VIS-NIR, used as waveguide for the light source excitation and for the detection
of the resulting back-scattered light.
A critical point on the Raman spectrometers is the filtering of the pump wavelength
by using a notch filter with the same wavelength of the pump wavelength. In this
work a notch filter NF785SF-33 was fixed between two micro-positioners PAF-SMA-5-B coupled to the optical probe used for the backscattered detection.
Finally, for the detection of the Raman signal, an optical fiber connected to the
micro-positioner was connected to a general-purpose commercial spectrometer USB4000-VIS-NIR (Table I).
TABLE I Commercial spectrometer configuration.
Specifications |
Specifications |
Wavelength Range |
693 nm |
Slit |
25 um |
FWHM |
1.42 nm |
Grating |
600 gr/mm |
Pixel Resolution |
7.5 |
Detector Elements |
3648 |
Blaze |
500 nm |
Input Focal
Distance |
42 mm |
Output Focal
Distance |
68 mm |
SNR |
300:1 |
The main parameters needed to customize a commercial spectrometer as a Raman
spectrometer are: the slit, the grating, the optical resolution and the spectral
range. The slit is defined as the input aperture of the spectrometer. In this part,
the incident beam from of light incoming from the optical probe is transmitted
inside the spectrometer divergently to a collimator and subsequently diffracted and
focused onto a CCD for detection. From the slit diameter and the pixel resolution,
it is possible to derive the slit diffractive angle of the spectrometer by using the
Young equation, resulting in an angle of 13.27∘. The grating is an optical periodic array of diffractive elements
impressed on a refractive surface, whose main purpose is to modify the magnitude or
phase of a beam of light. The capacity of the grating to diffract a beam of light is
ruled by the grating Eq. (2):
sinθi+sinθd=mλd
(2)
Where λ is the wavelength of the incident beam of light, m is the order of diffraction. In this work, the selected spectrometer has
a Blazed Grating, defined as a concentration of a limited zone designed to obtain a
mayor efficiency of a specific wavelength by the Eq. (3):
mλ=2dsinθB
(3)
Where θB is the blaze angle and is the angle formed between the face of the
groove and the grating plane. The blaze angle of the spectrometer was fixed at 13.65∘ and configured to have a maximum efficiency at 500 nm with a groove
period of 1.66 um. For the optical resolution or Full Width at Half Maximum (FWHM), defined as the capacity of the spectrometer for differentiating two
bands, it is needed that the parameters of the slit and the grating were efficiently
configured because a) greater the groove frequency of the grating, greater the
optical resolution, but resulting in a lesser spectral range. To determine the
optical resolution of the spectrometer, first it is necessary to derive the
dispersion by the wavelength range and the number of detectors of the spectrometer
following the Eq. (4):
D=RND
(4)
Where D is the dispersion, R the optical range and ND is the number of detectors. With the dispersion it is possible to
calculate the optical resolution with the Eq.
(5):
OR=DPR
(5)
Where OR is the optical resolution and PR is the pixel resolution. Because the grating and the slit were fixed,
the resulting values for this work were a dispersion of 0.189 nm/pixel and an
optical resolution of 1.42 nm. Finally, the spectral resolution, defined as the
separation between two spectral bands in function of the incident light wavelength
is ruled by the Eq.(6):
Δ1,2=λ0-OR
(6)
Where Δ1 and Δ2 are the differences between the incident light beam wavelength λ0 and the optical resolution
3. Results
Before the Raman detection, a wavelength detection characterization of the
spectrometer was performed in order to obtain the detection percentage of the
wavelength selected as a light source. For this task, a white-light tungsten lamp
Ocean Optics LS-1 was connected directly to the spectrometer and it could be seen that at
785 nm the percentage of detection of the spectrometer was of 54.11 (Fig. 2).
Following the proposed methodology in the Sec. 2, an optical resolution of 23 cm-1 was obtained, therefore, an effective characterization of the system was
performed on samples with characteristic Raman bands like the Si, which has typical Raman bands at 300 cm -1 and 521 cm -1 previously reported and available in the web [11] and was used as reference spectrum in this work. The
sample was put under the probe and the integration time was set to 10 s. Five Raman
spectra of the Si were obtained from the experimental Raman system and five spectra from
an Ocean Optics IDRaman Mini is shown in the Fig.
3, where it can be seen the considerable difference in the width between
the spectrums (Fig. 4). With this issue, the
possibility of quantitative analysis by comparing the resulted spectra with some
spectra from a data base is not possible, the possibility of a quantitative
analysis, by comparing the resulting pectra with some spectra from a data base is no
possible. insstead, it is only possible to perform a qualitative analysis of the
spectra by identifying bands.
The configuration of the Ocean Optics IDRaman Mini is the following: a laser diode of
90 mW as a light source, a spectral range of 400-2,300 cm-1 and a spectral resolution of 8 cm-1. Compared with this device, the experimental Raman system implemented
was considered as a low-resolution system capable of detect the Raman scatterings of
the sample under test.
4. Conclusion
Raman spectroscopy is a well-recognized technique used for material characterization,
illegal substances identification and recently, as a tool for medical diagnosis.
Unfortunately, the prices of the Raman systems are thousands of dollars making them
inaccessible for great part of the medical personal, also the largest dimensions of
the fixed Raman systems are a drawback for its heavy use. Actually, there are
several portable Raman systems, but again, the price and the performance are two
problems.
In this work, a methodology of design for an experimental Raman spectrometer is
presented and implemented, due to the lack of specificity in the components, the
results show a spectrometer with low resolution but capable of the detecting the
Raman bands of commonly used materials like silicon. It is from our great interest
in a future work to build a multi-purpose Raman spectrometer following the same
methodology of design described in this work, but with different and more accurate
components.
Acknowledgements
The authors thanks Dr. Edgar Guevara and Dr. Gabriel González for his critical
reading of the manuscript. F.S. Chiwo acknowledges support from CONACYT through
scholarship No. 559382. The authors also acknowledge support from CONACYT and the
National Labs program through LANCYTT, the Terahertz Science and Technology National
Lab. F. J. González would like to acknowledge support from Project 32 of “Centro
Mexicano de Innovación en Energía Solar”.
References
1. C V. Raman, Nature 108 (1921)
367.
[ Links ]
2. J.R. Ferraro, K. Nakamoto, and C. W Brown, Introductory
Raman Spectroscopy (2003).
[ Links ]
3. Ewen Smith and Geoffrey Dent. Modern Raman Spectrocopy: A
Practical Approach. (2005).
[ Links ]
4. Ian R. Lewis, Handbook of Raman Spectroscopy.
Marcel Dekker, Inc., (2001).
[ Links ]
5. Valery Tuchin, Tissue Optics, Light Scattering Methods
and Instruments for Medical Diagnosis, 39 (2008).
[ Links ]
6. P Naglic, Raman spectroscopy for medical
diagnostics., (2012) p. 1-9.
[ Links ]
7. R Richards-Kortum and E. Sevick-Muraca, Annu. Rev. Phys.
Chem. 47 (1996) 555-606.
[ Links ]
8. M. Gnyba, J. Sumulko, A. Kwiatkowski, and P. Wierzba.
Portable Raman Spectrometer-Design Rules and Applications.
Bulletin of The Polish Academy of Sciences, (2011).
[ Links ]
9. F.J. Gonzalez. Noninvasive detection of filaggrin
molecules by raman spectroscopy. In Filaggrin.
(2014).
[ Links ]
10. M. Ghebre Ramirez-Elias and F. Javier Gonzalez. Raman
Spectroscopy for In Vivo Medical Diagnosis. In Raman Spectroscopy.
IntechOpen, (2018).
[ Links ]
11. RRUFF Database of Raman Spectroscopy, X-Ray
Diffraction and Chemistry of Minerals. Online.
[ Links ]