Given a time stack of images, number()
performs a calculation of the number
for each pixel.
number(
img,
def,
thresh = NULL,
detrend = FALSE,
quick = FALSE,
filt = NULL,
s = 1,
offset = 0,
readout_noise = 0,
gamma = 1,
parallel = FALSE
)
A 4-dimensional array of images indexed by img[y, x, channel, frame]
(an object of class ijtiff::ijtiff_img). The image to perform the
calculation on. To perform this on a file that has not yet been read in,
set this argument to the path to that file (a string).
A character. Which definition of number do you want to use, "n"
or "N"
?
The threshold or thresholding method (see
autothresholdr::mean_stack_thresh()
) to use on the image prior to
detrending and number calculations. If there are many channels, this may be
specified as a vector or list, one element for each channel.
Detrend your data with detrendr::img_detrend_rh()
. This is
the best known detrending method for brightness analysis. For more
fine-grained control over your detrending, use the detrendr
package. If
there are many channels, this may be specified as a vector, one element for
each channel.
FALSE
repeats the detrending procedure (which has some inherent
randomness) a few times to hone in on the best detrend. TRUE
is quicker,
performing the routine only once. FALSE
is better.
Do you want to smooth (filt = 'mean'
) or median (filt = 'median'
) filter the number image using smooth_filter()
or
median_filter()
respectively? If selected, these are invoked here with a
filter radius of 1 (with corners included, so each median is the median of
9 elements) and with the option na_count = TRUE
. If you want to
smooth/median filter the number image in a different way, first calculate
the numbers without filtering (filt = NULL
) using this function and then
perform your desired filtering routine on the result. If there are many
channels, this may be specified as a vector, one element for each channel.
A positive number. The \(S\)-factor of microscope acquisition.
Microscope acquisition parameters. See reference Dalal et al.
Factor for correction of number \(n\) due to the illumination
profile. The default (gamma = 1
) has no effect. Changing gamma will have
the effect of dividing the result by gamma
, so the result with gamma = 0.5
is two times the result with gamma = 1
. For a Gaussian illumination
profile, use gamma = 0.3536
; for a Gaussian-Lorentzian illumination
profile, use gamma = 0.0760
.
Would you like to use multiple cores to speed up this
function? If so, set the number of cores here, or to use all available
cores, use parallel = TRUE
.
A matrix, the number image.
Digman MA, Dalal R, Horwitz AF, Gratton E. Mapping the Number of Molecules and Brightness in the Laser Scanning Microscope. Biophysical Journal. 2008;94(6):2320-2332. 10.1529/biophysj.107.114645.
Dalal, RB, Digman, MA, Horwitz, AF, Vetri, V, Gratton, E (2008). Determination of particle number and brightness using a laser scanning confocal microscope operating in the analog mode. Microsc. Res. Tech., 71, 1:69-81. 10.1002/jemt.20526.
Hur K-H, Macdonald PJ, Berk S, Angert CI, Chen Y, Mueller JD (2014) Quantitative Measurement of Brightness from Living Cells in the Presence of Photodepletion. PLoS ONE 9(5): e97440. 10.1371/journal.pone.0097440.
# NOT RUN {
img <- ijtiff::read_tif(system.file("extdata", "50.tif", package = "nandb"))
ijtiff::display(img[, , 1, 1])
num <- number(img, "N", thresh = "Huang")
num <- number(img, "n", thresh = "tri")
# }
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