DEFLECTION-TYPE REFRACTOMETER WITH EXTENDED MEASUREMENT RANGE

Abstract

A deflection-type refractometer with extended measurement range having, a light source generating a beam of light; a measuring cell with a sample chamber receiving a sample liquid; an optical sensor mounted on a movable platform for detecting the deflected beam of light; a driving unit configured to move the platform; a distance measurement unit for monitoring the displacement of the platform; a control unit configured to calculate the deflection of the beam of light based on the displacement of the platform and an output signal of the optical sensor to obtain a refractive index measure of the sample liquid using the calculated deflection.

Claims

1.-25. (canceled)

26. A deflection-type refractometer with extended measurement range for obtaining a refractive index measure of a flowing sample liquid, comprising: means for generating a beam of light, said means comprising a light source; a measuring cell comprising a sample chamber with inlet and outlet ports for receiving a flowing sample liquid, the measuring cell arranged such that the beam of light from the light source impinges on the sample chamber and is deflected after traversing two non-parallel faces of the sample chamber; an optical sensor mounted on a movable platform for detecting the deflected beam of light, wherein the optical sensor is a position sensing detector; a driving unit configured to move the platform; a distance measurement unit for monitoring the displacement of the platform; and a control unit comprising a data processing unit configured to: continuously calculate the deflection of the beam of light based on the displacement of the platform and an output signal of the optical sensor; and obtain a refractive index signal over time of the sample liquid using the calculated deflection.

27. The refractometer of claim 26, wherein the driving unit is configured to move the platform such that the deflected beam of light is centered at the optical sensor.

28. The refractometer of claim 27, wherein the processing unit of the control unit comprises a PID controller for continuously controlling the displacement of the platform.

29. The refractometer of claim 28, wherein the position sensing detector is a split photodiode formed by two individual photodiodes, wherein the driving unit is configured to move the platform such that the deflected beam of light is centered at the split photodiode, and wherein the error signal (e) of the PID controller is proportional to the difference between both individual photodiode output signals (A, B) and the applied action (u) is the displacement of the platform required to cancel out the error signal (e).

30. The refractometer of claim 26, wherein the driving unit is configured to move the platform according to a predetermined movement pattern.

31. The refractometer of claim 30, wherein the predetermined movement pattern is a continuous movement between two predefined positions at a constant speed or an arbitrary movement at time varying speed.

32. The refractometer of claim 26, wherein the position sensing detector is a split photodiode formed by two individual photodiodes, a lateral effect photodiode or a photodiode array.

33. The refractometer of claim 26, wherein the driving unit is configured to move the platform linearly.

34. The refractometer of claim 26, wherein the measuring cell is a body comprising a single chamber.

35. The refractometer of claim 26, wherein the measuring cell comprises a reference chamber for receiving a reference liquid, the measuring cell being arranged such that the beam of light is deflected after traversing two non-parallel faces of the reference chamber and sequentially traverses both the reference chamber and the sample chamber; and wherein the refractive index signal is the difference in refraction indexes (□n) between sample and reference liquids.

36. A gradient liquid chromatography system, comprising: the refractometer according to claim 35; a pump for pumping a mobile phase comprising a mix of two or more solvents into the reference chamber of the refractometer; a chromatography column, the output of which is connected to the sample chamber of the refractometer; and an injector for dosing a solute into the chromatography column.

37. A method for obtaining a refractive index measure of a flowing sample liquid, comprising: generating a beam of light; receiving a sample liquid in a sample chamber of a measuring cell with inlet and outlet ports for receiving a flowing sample liquid, the measuring cell being arranged such that the beam of light impinges on the sample chamber and is deflected after traversing two non-parallel faces of the sample chamber; moving a platform to detect the deflected beam of light using an optical sensor mounted on the platform, wherein the optical sensor is a position sensing detector; monitoring the displacement of the platform; continuously calculating the deflection of the beam of light based on the displacement of the platform and an output signal of the optical sensor; and obtaining a refractive index signal over time of the sample liquid using the calculated deflection.

38. The method of claim 37, wherein the platform is moved such that the deflected beam of light is centered at the optical sensor.

39. The method of claim 38, further comprising continuously controlling the displacement of the platform using a PID controller.

40. A gradient liquid chromatography method, comprising: pumping a mobile phase comprising a mix of two or more solvents into the reference chamber of a refractometer; dosing a solute into a chromatography column, the output of which is connected to the sample chamber of the refractometer; obtaining a refractive index signal over time of the sample liquid according to the method of 37.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0051] A series of drawings which aid in better understanding the invention and which are expressly related with an embodiment of said invention, presented as a non-limiting example thereof, are very briefly described below.

[0052] FIG. 1 shows a deflection-type refractometer according to the prior art.

[0053] FIGS. 2A and 2B depicts two embodiments of a deflection-type refractometer with a single-chamber flow cell according to the present invention, and FIG. 2C depicts a simplified view of another embodiment.

[0054] FIG. 3 depicts another embodiment of the refractometer, in this case with a double-chamber flow cell.

[0055] FIG. 4 depicts the use of a double-chamber cell in batch mode (FIG. 4A), single-chamber flow cell with continuous flow (FIG. 4B), double-chamber flow cell with static reference chamber and continuous flow though the sample chamber (FIG. 4C) and double-chamber flow cell with continuous flow through both chambers connected in series, before and after injector and column (FIG. 4D).

[0056] FIG. 5 shows the change in the incidence angle of a beam of light at the interface of two media with different refractive indexes.

[0057] FIGS. 6A, 6B and 6C depict three embodiments of the controller used by the refractometer.

[0058] FIGS. 7A and 7B show data from the refractometer of the present invention used with 1,2,4-trichlorobenzene (TCB), 1-decanol and mixtures thereof as mobile phase.

[0059] FIG. 8 is a graph showing the measured shift vs refractive index of the mobile phase for the experiment of FIGS. 7A and 7B.

[0060] FIGS. 9A and 9B shows the refractive index recorded continuously along the time scale from injections of a small amount of xylene in a mixture of different proportions of 1-decanol and TCB.

[0061] FIG. 10 shows the shift (deflection of the light beam) for a gradient Di-ethylene-glycol-mono-butyl ether (DEGMBE)—TCB.

[0062] FIG. 11A shows the shift for repeated injections of xylene along a continuous gradient 1-decanol—TCB. FIGS. 11B and 110 show an enlarged view of the same data during the first part and the last part of the gradient, respectively.

[0063] FIGS. 12A and 12B respectively depicts the recorded shift and the calculated refractive index during a continuous linear gradient of acetonitrile to water.

DETAILED DESCRIPTION

[0064] The present invention refers to a deflection-type refractive index detector with high precision and a very large measurement range, that can be used for liquid chromatography.

[0065] FIG. 1 depicts a deflection-type refractometer 100 according to the prior art, in which a beam of light 102 is generated from a light source 110 and a slit 120. The beam of light 102 impinges a dual-chamber flow cell 130 comprising two triangular prisms, a reference chamber 132 and a sample chamber 134, having inlet and outlet ports (not depicted in the figure) and respectively filled with reference liquid and flowing sample liquid with different refractive indexes n1 and n2. When the beam of light passes through the flow cell 130, it is deflected a certain angle a according to the differential refractive index (Δn=n2−n1) of both liquids.

[0066] The deflected beam of light 104 is detected by a split photodiode 140 placed at a fixed distance L from the flow cell 130. In particular, the displacement of the beam d is measured by the split photodiode 140, the deflection angle a is then obtained (α=tan.sup.−1 (d/L)) and the refractive index difference (n.sub.2−n.sub.1) is finally computed. If the difference is such that the displacement of the beam d at the detector plane is larger than the size H of the detecting device in the same dimension, the system is out of range. Typically, the maximum range in differential refractive units is around ±0.6.Math.10.sup.−3 DRIU (differential refractive index units).

[0067] In deflection-type refractive index detectors a beam of light is directed at a certain angle, typically 45° to the surface of a glass in contact with the sample liquid to be monitored.

[0068] According to Snell's law, the angle of the light beam after traversing the glass containing the sample liquid is different to the incidence angle and it is related to the refractive index of the media in contact at that surface, that is, the sample liquid to be monitored and the glass material of the container.

[0069] According to the prior art, the refractometers applied to liquid chromatography employ a two-chamber flow cell, with one of the chambers filled with the sample liquid (solvent plus solute), and the second chamber filled with a reference liquid (pure solvent), so there are two surfaces at which refraction takes place. If same liquid (pure solvent) is present in both chambers the angle of the beam of light after the dual-chamber cell is not modified, while a small change in refractive index of the liquid in one of the chambers due to the presence of some solute produces a small change in the angle of the beam of light after the flow cell. This change in the angle is detected at a certain distance L as a change in the position of the beam in the plane of a position sensing detector (i.e. displacement d). The displacement of the beam d, measured by split diode 140, is approximately proportional to the refractive index difference n.sub.2−n.sub.1, which in turn is proportional to the concentration of solute in the solvent of the sample liquid. The refractometers of the prior art normally include also a zero glass deflector (not shown in FIG. 1) to accurately adjust the deflected beam of light at the center of the split photodiode when the condition of Δn=0 is set.

[0070] This system works only for small differences in refractive index, which generate small angular variations. However, in gradient liquid chromatography, when two different solvents (of different polarity) are combined to form the mobile phase in time-varying proportion, the change in refractive index of the mobile phase is orders of magnitude larger that the differences caused by a solute in a solvent, so the variation of the deflection angle along the gradient analysis is much larger than the possible measurement range (limited by the size H of the detecting device). These refractometers are therefore not useful when used in gradient liquid chromatography analysis.

[0071] The refractometer of the present invention is especially useful for gradient liquid chromatography since it possesses a large measurement range in refractive index units (RIU), which can follow the continuous change in refractive index when the mobile phase composition is varied from one solvent to the other. In the present invention the position sensing detector (split diode) is placed on a moving platform, so that it is able to measure very large displacement values d, in the order of centimeters, which translate at least in tenths of RIU units of refractive index change.

[0072] FIG. 2A represents a deflection-type refractometer 200 according to an embodiment of the present invention. The refractometer 200 comprises means for generating a beam of light 202 that will be deflected by the sample liquid and impinge on the plane of the position sensing detector, generating a light beam image on that plane, which will move according to the deflection experienced by said light beam.

[0073] The beam of light 202 may be produced, for instance, using a light source 210, collimated such as a laser diode or non-collimated such as an LED or lamp with a collimating lens (not shown in the figure) and a restrictive light slit 220. Additional optical elements (e.g. lenses, slits, optical apertures) may be employed for the generation of the beam of light or beam image.

[0074] A measuring cell 230 comprises a sample chamber 234 containing a sample liquid. Two faces (front face 234a and rear face 234b) of the sample chamber 234, which are not parallel to each other, are traversed by the light beam so that when the beam of light 202 passes through the sample chamber 234 it is deflected by the sample liquid a certain angle. Those two faces need to be made of a material transparent to the wavelength of the light used, such as glass, fused silica, quartz, sapphire, for visible light, and also be polished to prevent diffuse reflection or scattering of the beam of light. The rest of the cell walls may be made from the same material or different as they do not interact with the light rays of interest. The deflected beam of light 204 is detected by a position sensing detector mounted on a movable platform 240. The position sensing detector is preferably implemented as a split photodiode 242 formed by two individual photodiodes (242a, 242b) or, alternatively, as a lateral effect photodiode of adequate sensitivity or other known position sensitive device such as a photodiode array.

[0075] The refractometer also comprises a driving unit 254 configured to move the platform, a distance measurement unit 260 configured to measure the displacement of the platform 240 and a control unit 250 that receives the output signal 244 from the position sensing detector (e.g. the signal coming from each individual photodiode 242a and 242b). The distance measurement unit 260 detects each minimal displacement of the platform 240 with high resolution, preferably in the order of submicrons or nanometers (any known detector may be used to that end). The distance measurement unit 260 may be an element integral to the driving unit 254 (e.g. optical encoder of a motor), as in the example of FIG. 2A, or an element external to the driving unit 254, as shown in the embodiment of FIG. 2B. The control unit 250 comprises a data processing unit 252, implemented for instance as a microcontroller or a computer, that calculates the deflection of the beam of light (deflection angle a caused by the measuring cell 230) based on the displacement of the platform 240 and the output signal 244 of the position sensing detector, thereby obtaining a refractive index measure of the sample liquid inside the sample chamber 234 using the calculated deflection. The control unit 250 may obtain the displacement of the platform 240, for instance, directly from the driving unit 254 (e.g. using an encoder thereof) or using an external sensor (not shown in the figure) configured to monitor the positioning of the platform 240. In either case the resolution in the displacement is preferably in the order of nanometers, in order to provide the required resolution in refractive index units.

[0076] In the embodiment shown in FIG. 2A, the driving unit 254 moves the platform 240 linearly along an axis H perpendicular to the beam of light 202 (in the example, the beam of light 202 is a horizontal line and the axis H is a vertical line). Instead of a linear movement, the driving unit 254 may move the platform 240 following a known trajectory, for instance an angular movement, such that the position of the platform 240 can be determined at each instant.

[0077] The driving unit 254 may be an entity external to the control unit 250, as depicted in FIG. 2A. Alternatively, as shown in the embodiment of FIG. 2B, the driving unit 254 may be part of the control unit 250.

[0078] In an embodiment, the driving unit 254 independently moves the platform according to a predetermined movement pattern, for instance a continuous movement between two pre-defined positions at a constant speed, or some arbitrary movement at time varying speed. The driving unit 254 may instead be controlled by an activation instruction 256 sent by the data processing unit 252 of the control unit 250.

[0079] In the embodiment of FIGS. 2A and 2B, the measuring cell 230 is a single-chamber cell, in particular a triangular prism with a single chamber (the sample chamber 234), wherein the triangular prism is arranged such that the incidence angle of the beam of light 202 is 90° at an external, front face of the prism. In another embodiment depicted in FIG. 2C (not showing the control unit 250 and driving unit 254) a single-chamber measuring cell 230 is arranged in a position such that the incidence angle of the beam of light 202 is not normal to the first surface (front face 234a), and therefore there are two surfaces (front face 234a and rear face 234b) at which the beam is deflected when traversing the measuring cell 230. FIG. 3 depicts a refractometer 300 according to yet another embodiment, in which the measuring cell 330 is not a single-chamber cell, but a dual-chamber cell. In this case the measuring cell 330 comprises a sample chamber 334 for receiving a sample liquid and also a reference chamber 332 for receiving a reference liquid. The measuring cell is arranged such that the beam of light is deflected after traversing two non-parallel faces (front face 332a and rear face 332b) of the reference chamber 332 and then two non-parallel faces (front face 334a and rear face 334b) of the sample chamber 334. The refractive index computed by the data processing unit 252 is the difference in refraction indexes (Δn) between the sample liquid (refraction index n2) and the reference liquid (refraction index n1).

[0080] FIG. 4A illustrates the operation of the measuring cell in a refractometer as a batch detector. The reference chamber of the cell is filled with a reference liquid whose refractive index is known, and then the reference chamber is sealed. The sample chamber is filled with a sample liquid whose refractive index is unknown (alternatively, the sample liquid may be flowing through the sample chamber). In that situation the differential refractive index of the sample liquid with respect to the reference liquid is measured by the detector. The reference chamber can also be omitted in the refractometer of the present invention (not shown in FIG. 4A); in that case, the absolute refractive index of the sample liquid is measured.

[0081] Possible implementations for operation of the refractometer of the present invention as online analyzer in a chromatograph (or similar system) is illustrated in FIGS. 4B to 4D. FIG. 4B depicts a chromatograph using a single-chamber flow cell refractometer with continuous flow, FIG. 4C depicts a double-chamber flow cell with static reference chamber and continuous flow though the sample chamber, and FIG. 4D depicts a double-chamber flow cell with continuous flow through both chambers connected in series.

[0082] As depicted in FIG. 4C, the reference side of the cell may be filled with a reference fluid, using the reference inlet (471) and reference outlet (472) and then sealed by means of the reference closure element (473). This way the reference fluid is kept static along the use of the detector, while a continuous flow of sample liquid is kept through the sample chamber 334. The difference in refractive index over time between the flowing liquid in the sample chamber and the stagnant liquid in the reference chamber is calculated and produced as detector output to be recorded. This difference in refractive index increases continuously as the refractive index of the fluid flowing only through the sample chamber changes, since the refractive index of the fluid in the reference chamber is fixed. This translates in an increasing deflection angle and so an increasing displacement required for the moving platform.

[0083] Alternatively, the reference chamber 332 of the cell can be connected in series with a flowing liquid, as depicted in the refractometer 400 of FIG. 4D. To that end, the reference chamber comprises inlet 412 and outlet 414 ports for receiving the flowing reference liquid 410. The dashed arrows indicate the direction of flow. When a mobile phase 408 of time-varying composition, produced continuously by mixing of two or more different solvents (first solvent 402, second solvent 404), is pumped though the system (by the action of a pump 406), it reaches first the reference chamber 332 (i.e. the reference liquid 410 of the reference chamber 332 is the mobile phase 408 used in liquid chromatography); then, after some delay time due to the volume in an injector 420, system tubing and column 430 (one or several, if any), the sample liquid 440, containing a mobile phase (408) mix of solvents (402, 404) and eventually a solute from the injector 420, reaches the sample chamber 334 of the measuring cell 330. The sample chamber 334 comprises inlet 416 and outlet 418 ports through which the sample liquid 440 flows.

[0084] Due to the volume delay between reference and sample chambers, the mobile phase composition in the reference liquid and sample liquid is different, and so there is a difference in refractive index between the liquid of the two chambers due to the mobile phase composition change over time. In addition, when a solute loaded into the injection loop (425) by some means (not shown) is injected into the mobile phase stream by the injector (420), traverses the column (430) if any, and enters the sample chamber (334) in the flow cell of the refractometer, there is an additional difference in refractive index between the liquids in the two chambers due to that solute. This additional difference is not constant over time but is only present while the solute traverses the sample chamber, and typically is very small compared to the difference due to the different composition in mobile phase. In this configuration, the refractive index of the fluids within each of the two cell chambers (332, 334) is not fixed but time-varying according to the time-variations of the pumped mobile phase 408. The difference in refractive index does not increase continuously as in the case of a stagnant reference cell, but it remains limited within a certain interval. The width of that refractive index interval is defined by the volume delay between both chambers, flow rate through the system and rate of change of composition in the mobile phase, as well as on the difference in refractive index of the components of the mixture.

[0085] In particular, when a linear solvent gradient is applied, the difference in refractive index between the two chambers of the cell would remain approximately constant. Using the configuration of FIG. 4D the difference in refractive index between the two chambers in the cell is limited and therefore the angular deflection and the displacement required for the moving platform is also limited. This may be advantageous to minimize the size of the detector and could be used to enhance the sensitivity or resolution of the detector.

[0086] The angle formed by the two faces of the cell, and the incidence angle of the beam of light on the first cell face determine the magnitude of the deflection angle after the cell for a given refractive index of the fluid or fluids in the cell (single or double chamber cell cases), according to the Snell law, applied to each of the interfaces traversed consecutively by the light beam. In particular, the following relation is fulfilled: sin ∝.sub.1.Math.n.sub.1=sin ∝.sub.2−n.sub.2, where ∝.sub.1 and ∝.sub.2 are the angles of incidence at the interface and n.sub.1 and n.sub.2 are the indices of refraction of the media. In the case of normal incidence, the deflection angle is zero for any refractive index, and the lower the incidence angle (farther from the normal incidence) the larger the deflection due to a change in the refractive index of the fluid in the cell. In FIG. 5, given n.sub.1 and n.sub.2 the refractive indexes of the two media, for an incidence angle α.sub.1, the angle of the deflected beam is α.sub.2. When the refractive index of the second medium changes to n.sub.2+Δn, the angle of the deflected angle changes to α.sub.2+Δα. For a given change in refractive index Δn, the change in deflection angle Δα is larger when α.sub.1, as defined in FIG. 5), is larger.

[0087] When going from a medium of larger refractive index to a medium of lower refractive index, the incidence angle cannot be lower than the critical angle at which no refracted light is transmitted. When varying the incidence angle and/or the angle formed by the two faces of the measuring cell, the change in deflection angle for a change in refractive index can be increased, or maximized, thus increasing the sensitivity of the detector to refractive index changes. Since the refractometer of the present invention is able to measure a larger range of deflection angles than refractometers of the prior art, maximizing the deflection angle beyond the limit imposed by the physical dimensions of the split diode is possible and desirable. Therefore, the incidence angle of the beam of light can be optimized to maximize the deflection within the available measurement range, in order to maximize the sensitivity.

[0088] When the light traverses an interface between two media, and the refractive index of the first one is higher than the refractive index of the second one, there is an incidence angle at which the deflection angle calculated according to Snell's law is 90°. This is called the critical incidence angle or critical angle and beyond that critical angle there is no refracted light but only total reflection. An incidence angle close to the critical angle provides the maximum change in deflection angle Δα, for a given change in refractive index Δn, so a configuration with an incidence angle close to the critical angle is preferred when enhancing the sensitivity is prioritized over extending the range in refractive index units, so that the deflection angle variation due to refractive index variation is maximized.

[0089] In an embodiment, the platform is moved by the driving unit 254 such that the deflected beam remains within the physical limits of the split photodiode 242. An embodiment for a controller which can operate as described is depicted in FIG. 6A. This controller is a speed controller 257 that monitors the individual signals of the photodiodes A and B in order to move the platform so that the beam image does not move beyond the physical limits of the split photodiode. The total deflection of the beam (from which the refractive index of the fluid is calculated) is obtained from the known position of the moving platform and the difference between the signals of the two photodiodes. In one non-limiting implementation, the controller is programmed to decide the direction of movement depending on which photodiode generates a larger signal: when the image of the deflected beam of light moves in the direction of one of the photodiodes it covers a larger area of the same, and therefore the signal of that particular photodiode increases while the opposite is true for the other photodiode. In order to follow the direction of movement of the deflected beam, the platform needs to be moved in that same direction, indicated by the photodiode with larger signal. The movement only starts when the signal of the lower signal photodiode decreases under a preset level. The movement starts at an initial speed. If the signal goes over that preset level the movement stops again. The speed is increased if the signal decreases further and falls under a second predefined level. Every time the movement stops, the speed is reset to its initial value. The purpose of the outline controller is to track the movement of the beam only to prevent it moves out of the split photodiode, so that the relative position of the beam to the split photodiode position can be measured accurately overtime. That relative position together with the known position of the platform are used to compute the total deflection of the beam and the refractive index of the fluid in the sample chamber.

[0090] In a preferred embodiment, the platform is moved by the driving unit 254 such that the deflected beam of light 204 is continuously centered at the split photodiode 242 (i.e. the center of the split photodiode 242 is continuously tracking the deflected beam of light 204). Therefore, the control unit 250 acts as a beam tracking digital servo-controller. To that end, the processing unit 252 of the control unit 250 may comprise a PID controller 258 (as depicted in the embodiment of FIG. 3) for continuously controlling the position of the platform so that the deflected beam of light 204 is centered at the split photodiode 242. FIG. 6B depicts an embodiment of the PID controller 258 in which the input error signal (e) of the PID controller 258 is the difference between the output signals (A, B) of both individual photodiodes (242a, 242b). The error signal (e) may be a proportional signal of said difference (A−B), for instance the normalized difference defined as A−B/A+B.

[0091] The output (u) of the PID controller 258 is the displacement of the platform 240 required to cancel out the error signal (e). The output (u) corresponds to the activation instruction 256 sent to the driving unit 254, which in turn, from its current position, moves up or down the movable platform a magnitude according to said activation instruction 256.

[0092] The error signal required for the PID controller operation may also be implemented from the outputs of alternative position sensing, such as a lateral effect photodiode or a sensor array. The output of such alternative devices could be either analog or digital but still proportional to the distance of the beam position to the center of the detector, with opposite sign depending on the direction of the unbalance.

[0093] In another embodiment depicted in FIG. 6C, the platform 240 is moved by the driving unit 254 such that the deflected beam position is tracked by means of a light power sensor 248 whose output signal 244 is maximum when said light power sensor 248 is perfectly aligned with the beam. A signal maximization controller 259 is used to calculate the magnitude and sense (positive or negative) of the movement required for such perfect tracking based on the current and past values of the light power sensor output signal 244 and the previous and current positions of the platform. The output (u) of this signal maximization controller 259 corresponds to the activation instruction 256 sent to the driving unit 254, which in turn, from its current position, moves up or down the movable platform 240 a magnitude according to said activation instruction 256. In this embodiment the light beam deflection is obtained by the position of the platform 240.

[0094] The refractometer of the present invention is preferably applied in liquid chromatography or related techniques, using either an isocratic or a gradient elution. The measuring cell is a flow cell, and the sample chamber 234 comprises inlet and outlet ports for receiving a flowing sample liquid coming from the column chromatography. In the embodiment of FIG. 3, the measuring cell 330 may be a flow cell of the type used in liquid chromatography, wherein both the sample chamber 334 and the reference chamber 332 comprises inlet and outlet ports for receiving a flowing sample liquid (solvent plus solute coming from the column chromatography) and a reference liquid (pure solvent), respectively.

[0095] In an embodiment, the movable platform 240 is driven by a high-resolution motor stage able to perform and monitor movements in nanometer scale (for instance a piezo motor stage). This very high resolution allows determination of very small differences in refractive index which is required for accurate quantification of concentration of solutes in liquid chromatography or any other application demanding such a large measurement range in the refractive index.

[0096] The combination of large movement range and high resolution provides a new approach to measure refraction index and allows the use of the new detector in applications such as gradient liquid chromatography, in which conventional refractometers cannot be used. According to a preferred embodiment used in liquid chromatography, a servo-control (control unit 250) adjusts the motor position (driving unit 254) so that the deflected light beam is always centered at the split diode, generating a zero output. In an embodiment, a proportional derivative integral (PID) algorithm is implemented by the data processing unit 252 of the control unit 250 to allow the system continuously track the position of the beam with high accuracy. The PID controller 258 takes as input the split diode signal, which is zero when the beam is centered on it, and positive or negative depending on the position of the beam respect to the split diode center.

[0097] The PID controller 258 is optimized by measuring the dynamic response of the system by proper controlled experiments. One of such experiments involves a step movement of the motor and monitoring of the response of the split diode as a function of time. From this experiment, the dynamic characteristics of the system can be extracted for calculation of the optimized controller (i.e. values of P, I, D coefficients). Alternative controllers which can be optimized to the dynamic behavior of the system can of course be used as well. If the controller is not properly optimized the system may become unstable and the motor oscillate around the actual position of the beam, or become unable to follow accurately fast changes in position. When there is a real change in refractive index due to the presence of a solute (a peak in the liquid chromatography experiment) the optimized PID controller 258 allows accurate tracking of the peak, without overshooting or smoothing.

[0098] As previously explained in FIGS. 2A and 2B, it is also possible to use a flow cell (i.e. measuring cell) with a single chamber, without the reference chamber. One of the purposes of the reference chamber of the flow cells in conventional refractometers is forcing the beam of light to a fixed zero position by filling the two chambers with same pure solvent. This is necessary due to the limited range in displacement which can be detected. In the refractometer of the present invention the range is large enough so that it is not necessary to bring the beam to the same “zero” position by optical means or by using a double chamber cell. Moreover, the absolute position of the motor when the single cell is filled with a given solvent allows to calculate the absolute refractive index of that solvent, at the cell temperature and wavelength of the light used to generate the beam. This way the detector can be considered an absolute refractive index detector.

[0099] In order to demonstrate the much broader range of the present invention compared to the prior art, which is large enough to cover practical applications of gradient liquid chromatography, a system described in literature is chosen as a test system. According to the paper “Separation of short-chain branched polyolefins by high-temperature gradient adsorption liquid chromatography”, Macko et. al Anal Bioanal Chem. 2011 February; 399(4):1547-56, the system 1-decanol/1,2,4-trichlorobenzene (TCB) can be used in gradient liquid chromatography mode for the separation of polyolefins depending on their chemical composition. In FIGS. 7A and 7B data from the refractometer of the present invention is presented when TCB, 1-decanol and mixtures thereof in different proportions covering the full range is flown through the measuring cell 230 as mobile phase at constant flow rate of 0.5 mL/min. The refractive index of TCB and 1-decanol can be taken as 1.572 and 1.436, so the total change in refractive index is 0.136 RIU, larger by orders of magnitude of what previous deflection-type detectors can measure. In the figures it is clear how the signal from the detector in units of shift (displacement of the platform in microns, μm) follows accurately, without saturation, the full range in composition of mobile phase as it is changed from TCB to 1-decanol in steps or 20% or 10%.

[0100] From the data in FIG. 7A and knowledge of refractive index of TCB and 1-decanol, and assuming that the refractive index of mixtures of the same is proportional to the volume fraction of the components, a series of data points, measured shift vs refractive index of the mobile phase, can be plotted, as depicted in FIG. 8. From the graph it is apparent that the measured shift and refractive index is almost linear.

[0101] The system was also tested by injecting a small amount (5 μL) of xylene which has a refractive index of 1.501, an intermediate value between those of 1-decanol and of TCB into a continuous stream of mobile phase flowing through the detector cell. Injections were made when a mixture rich in TCB (FIG. 9A) or rich in 1-decanol (FIG. 9B) were used as mobile phase. The mobile phase composition determines the baseline refractive index, that is, the constant level in the detector output when the mobile phase flows through the cell. When the test sample with a different refractive index enters the cell, the detector output changes to track the refractive index change, generating a peak in the detector output as seen in FIGS. 9A and 9B. When the refractive index of the test sample is lower than the baseline refractive index (1.501 for xylene compared to 1.544 of the TCB rich mobile phase), a negative peak is generated (FIG. 9A), while when the refractive index of the test sample is higher than the baseline level the resulting peak is positive, as in FIG. 9B (1.501 for xylene compared to 1.463 of the TCB rich mobile phase). Therefore, the background refractive index was over or below that of the injected sample, causing the sample peak to be negative or positive over the baseline.

[0102] In addition to the isocratic experiments using different mobile phase compositions depicted in FIGS. 7A and 7B, the operation in a continuous gradient of mobile phase compositional change is demonstrated in FIG. 10 (linear gradient Di-ethylene-glycol-mono-butyl ether (DEGMBE)—TCB).

[0103] FIGS. 11A, 11B and 11C show the operation of the detector when a test sample (5 microliter xylene) is injected multiple times along a continuous linear gradient 1-decanol—TCB flowing though the detector cell at a constant flow rate of 0.25 mL/min. Given the refractive index of xylene has an intermediate value between 1-decanol and TCB, the peaks during the first part of the analysis are negative (enlarged view in FIG. 11B) while the observed peaks during the last part of the gradient, are positive (FIG. 11C).

[0104] Even if the data in FIG. 8 show an almost perfect linearity, the refractive index of the mixture of two solvents does not necessarily follow a linear trend with the volume fraction of each of the components. A very clear example of this behavior is another system tested with the same refractometer: a gradient of acetonitrile to water in 60 minutes at a flow rate of a 0.3 mL/min with 10 minutes wait at the end was performed and data of observed shift (deflection of the light beam image after traversing the cell) is presented in FIG. 12A, and calculated refractive index in FIG. 12B. For this system the refractive index not only does not change linearly with the proportion of water, but it inverts the direction of variation, resulting in intermediate compositions with lower refractive index than any of the two components.