an optical frequency domain imaging (“ ofdi ”) systems with an a - line rates of 50 khz was used in this study . an exemplary embodiment of an ofdi system which can be used with the methods and arrangements according to the present invention is shown schematically in fig1 ( a ) . ( see , e . g ., b . j . vakoc et al ., “ phase - resolved optical frequency domain imaging ,” optics express 13 , 5483 - 5493 ( 2005 ); and s . h . yun et al ., “ high - speed optical frequency - domain imaging ,” optics express 11 , 2953 - 2963 ( 2003 )). for example , light from a swept source 100 can be split into a fiber optic reference arm 105 and a sample 110 preferably incorporating optical circulators 115 a , 115 b . a reflected light 121 from a sample 120 can be combined with a light 125 from the reference arm 105 in a free - space optical circuit utilizing a non - polarizing broadband beam splitter ( bbs ) 131 and polarization beam splitters ( pbs ) 132 a , 132 b . thus , both a balanced - detection and a polarization - diversity detection can be enabled . for example , a 1 % tap coupler 135 in the sample arm 110 can be used to generate a continuous phase recalibration signal which may allow for phase variations due to timing jitter to be removed . the imaging beam can be scanned across the sample with a high - speed galvanometer 140 , as shown in fig4 ( b ) a polarization controller ( pc ) 101 can be placed in the interferometer reference arm . an acousto - optic frequency shifter ( fs ) 102 was incorporated in the reference arm . multimode fibers ( mmf ) 141 may be used to couple the optical output signals to balanced receivers ( rx ) 142 . light was conveyed to the sample by a high - speed galvanometric beam scanner 143 . the acousto - optic frequency shifter 102 can be operated at about 25 mhz , and may be used to double the imaging range through the removal of depth degeneracy . ( see , e . g ., s . h . yun et al ., “ removing the depth - degeneracy in optical frequency domain imaging with frequency shifting ,” optics express 12 , 4822 - 4828 ( 2004 )). interference fringes may be digitized at about 100 ms / sec . as described above , an exemplary use of a laser source that sweeps asynchronously with the acquisition board digitization clock can produce a variability in both the starting time and the starting wavelength of each acquired a - line . the variability in the starting wavelength may result in a spurious , depth - dependent phase shift . the variability in the starting time in combination with the use of an acousto - optic frequency shifter may induce a spurious , depth - independent phase shift . it may be difficult to discern the relative contributions of a starting wavelength variation and a starting time variation using a single recalibration mirror signal . therefore , it may be difficult to determine how to scale the measured phase shift with depth to generate an appropriate correction signal . to address this , a modified phase recalibration approach can be implemented . for example , instead of a single phase recalibration signal , a pair of phase recalibration signals spaced approximately 100 microns apart can be generated from a reflection from a front surface and a back surface of a glass slide 137 . the following exemplary procedure can be used to remove spurious timing and starting wavelength induced phase shifts : ( a ) the phase difference between two recalibration signals can be measured , and the phase difference at zero differential depth may be determined by a linear extrapolation . fig2 ( a ) illustrates an exemplary measured a - line showing exemplary phase recalibration signals 200 a , 200 b . fig2 ( b ) shows an exemplary extrapolation of the measured phase difference from each signal 202 a , 202 b to that at a zero differential delay 201 . because the phase shift due to variations in the starting wavelength can scale with depth , the phase shift at zero differential delay therefore may provide such component resulting from the frequency shifter . further , by phase - locking the data acquisition clock ( e . g ., at about 100 mhz ) and the frequency shifter drive signal ( e . g ., at about 25 mhz ), the value of this exemplary phase variation may be restricted to an integer multiple of π / 2 ( 2π * 25 / 100 ). the extrapolated value may therefore be rounded to the nearest integer multiple of □/ 2 . this extrapolated phase shift can then be subtracted from the measured phase difference at all depths , possibly removing the errors resulting from the frequency shifter . fig2 ( c ) shows an exemplary distribution of measured phase shifts at zero differential delay ; and ( b ) after completion of exemplary procedure ( a ) above , same or similar approach previously described to remove phase shifts origination from the variations in the starting wavelength can be applied . the signal from either surface of the glass slide can be used as the phase recalibration signal . the generalization of the exemplary embodiment of a phase recalibration approach described above may provide for a phase - sensitive doppler imaging in the exemplary embodiment of ofdi systems incorporating a frequency shifter . an exemplary embodiment of a beam scan pattern can be used that may , in contrast to conventional ramp scan patterns , decouple a doppler integration window and an imaging frame rate by acquiring exemplary doppler measurements in parallel . as a result , high frame rate systems with extremely high doppler sensitivities can be achieved . the specific exemplary beam scan pattern discussed herein may have , e . g ., a segmented sawtooth waveform . for example , fig3 ( a ) illustrates one of the possible exemplary configurations of this scan pattern , and can define the relevant parameters of the exemplary scan . the overall scan pattern may comprise of a series of n identical concatenated segments ( e . g ., n = 8 as shown in fig3 ( a ) and 3 ( b ) ). each segment may acquire doppler measurements over a portion ( 1 / n ) of the full transverse field of view . within each segment , as illustrated in fig3 ( b ) , the beam can be scanned for p a - lines ( e . g ., p = 22 shown in fig3 ( a ) and 3 ( b ) ) at , e . g ., a constant velocity to provide a first phase measurement over such exemplary limited transverse extent . the beam can then be rapidly returned and allowed to stabilize over a series of m a - lines ( e . g ., m = 18 as shown in fig3 ( a ) and 3 ( b ) ), and subsequently rescanned over the same transverse extent previously sampled . measurements of exemplary phase shift between the first and second scan may provide the flow information , with the doppler integration window given by ( m + p ) a - lines . by changing the number of segments , n , in a given scan , this doppler integration time can be reduced or increased , as illustrated in fig3 ( c ) and 3 ( d ) which shows similar scans for ( n = 32 ) and ( n = 2 ) with correspondingly shorter and longer integration times . table 1 provided herein below can define several ( e . g ., seven ) scan patterns with a range of segments per frame ( n ) and corresponding doppler sensitivities . in these exemplary patterns , the number of a - lines per frame can be held constant at about 2048 , and the resulting image width may be held constant at 704 pts / pixels . additionally , 64 a - lines can be discarded from the beginning of each scan to allow for the flyback / settling time of the galvanometer between frames . the flyback time within the segments ( m ) can be scaled with the flyback distance , which may scale with the number of segments ( n ). taken together , these exemplary seven scan patterns can each be acquired at about 24 fps , and may provide the doppler sensitivity to be adjusted by a factor of about 64 . the measured phase sensitivities and minimum detectable flow velocities listed in table 1 are described herein . the scan patterns described in table 1 may be used to generate doppler images of size 704 × 1024 pixels using a 50 khz a - line rate system as described herein . an exemplary bulk motion can be removed by subtracting the median phase shift for points with a signal magnitude exceeding a given threshold . ( see , e . g ., m . c . pierce et al ., “ simultaneous intensity , birefringence , and flow measurements with high - speed fiber - based optical coherence tomography ,” optics letters 27 , 1534 - 1536 ( 2002 )). exemplary structural images may be generated as a mean of the a - line power reflectivity of each of the a - lines between which phases may be compared for the doppler image . the phase difference at each depth from the polarization channel with the largest signal may be used ; and the phase difference measured in the orthogonal channel can be discarded . because the doppler integration window can be increased , e . g ., almost arbitrarily with the segmented sawtooth scan pattern , the phase noise background does not have to play a limiting role in determining the doppler sensitivity . however , it may be important that this phase noise floor can be approximately independent of the doppler integration window to ensure that enhancements in sensitivity from the latter are not cancelled by increases in the former . to verify that the noise floor remained approximately constant , images of a homogenous rubber phantom may be acquired using each of the scan patterns described in table 1 , and the phase noise may be calculated as the standard deviation of the phase difference within a 500 × 280 pixel ( e . g ., 2 . 8 mm × 1 . 2 mm ) region of interest (“ roi ”). table 1 lists the exemplary measured phase noise for each scan pattern . the exemplary noise can remain approximately constant as the doppler integration time increases . the axial flow sensitivity predicted from the measured phase sensitivity by eq . 1 can also be provided to demonstrate the scaling of flow sensitivity with scan pattern parameters . to demonstrate the scaling of the doppler sensitivity with the scan pattern parameters , exemplary images of a flow channel phantom may be acquired for each of the patterns of table 1 and , e . g ., for three flow velocities . for example , the flow phantom may consist of a transparent sheath 400 embedded in a silicone rubber 401 with tio2 added to provide scattering . glycerol with the same tio2 scatters 410 can be effected to flow through the tube using an infusion pump with variable flow settings . fig4 ( a ) illustrates a portion of an exemplary structural image of the flow phantom , and fig4 ( b ) illustrates a corresponding exemplary doppler image . the flow within the tube may be clearly indicated in the doppler image , with the magnitude being large enough to induce phase wrapping as indicated by the rings . the exemplary embodiment of the system according to the present invention can be configured to rapidly alternate between each of the seven scan patterns in succession . exemplary doppler images for each of the patterns are shown in fig4 ( b ) , with each row presenting the images from each of the seven scan patterns for a fixed flow velocity , and each row showing these results for a different flow velocity . each exemplary image can be mapped to the same or similar grayscale of fig4 ( b ) . the scaling of the sensitivity within each row , and the consistency in the level of the phase noise background within each image are provided . the foregoing merely illustrates the principles of the invention . various modifications and alterations to the described embodiments will be apparent to those skilled in the art in view of the teachings herein . indeed , the arrangements , systems and methods according to the exemplary embodiments of the present invention can be used with imaging systems , and for example with those described in international patent application pct / us2004 / 029148 , filed sep . 8 , 2004 , u . s . patent application ser . no . 11 / 266 , 779 , filed nov . 2 , 2005 , and u . s . patent application ser . no . 10 / 501 , 276 , filed jul . 9 , 2004 , the disclosures of which are incorporated by reference herein in their entireties . it will thus be appreciated that those skilled in the art will be able to devise numerous systems , arrangements and methods which , although not explicitly shown or described herein , embody the principles of the invention and are thus within the spirit and scope of the present invention . in addition , to the extent that the prior art knowledge has not been explicitly incorporated by reference herein above , it is explicitly being incorporated herein in its entirety . all publications referenced herein above are incorporated herein by reference in their entireties .
an exemplary apparatus and / or an exemplary method can be provided using which , it is possible to measure an amplitude and / or a phase of at least one electromagnetic radiation provided from a particular portion of a sample . further , it is possible to scan a location of the particular portion along a path from a first point of the sample to a second point of the sample . in addition , it is possible to control the scan such that the scan may comprise at least one first segment having a positive velocity and at least one segment having a negative velocity . a first distance of the first segment and / or the second segment can be smaller than a second distance between the first and second points .