(a) Ordinary camera
(b) Variable exposure time
camera
Figure 3: The relationship between the input intensity E and
the measurements in the ordinary camera and the proposed
variable exposure time camera. The blue lines show image
intensity I in (a) and exposure time T in (b). The red line
in (a) shows the resolution
dI
dE
of image intensity I in the
ordinary camera, and the red line in (b) shows the resolution
dT
dE
of exposure time T in the proposed camera.
this imaging method, we accumulate input light at
each pixel, so that the accumulated image intensity
at the pixel becomes a certain constant value. This is
achieved by controlling the transmittance R(x, y, t) at
pixel (x, y) as follows:
R(x, y,t) =
1 I(x, y,t) < I
θ
0 otherwise
(7)
where I
θ
is a threshold, and I(x, y,t) is the accumu-
lated image intensity at pixel (x, y) up to time t as fol-
lows:
I(x, y, t) =
Z
t
0
Z
y+
1
2
y−
1
2
Z
x+
1
2
x−
1
2
R(x, y,t)L(u, v,t)dudvdt.
(8)
Then, we record the time t as the exposure time
T(x, y) of pixel (x, y), when R(x, y, t) changes from
1 to 0. In this imaging method, we control the ex-
posure time T(x, y) of each pixel, so that the accu-
mulated image intensity I(x, y) is under the threshold
value I
θ
. Thus, the over exposure does not occur in
this method. The intensity of input light is measured
as the exposure time unlike the standard camera. That
is the exposure time T(x, y) is inversely proportional
to the intensity of input light E(x, y) as follows:
T(x, y) =
I
θ
E(x, y)
(9)
Thus, unlike the ordinary cameras shown in Eq.(5),
the proposed imaging model measures the input light
intensity E(x, y) according to the following relation-
ship:
T(x, y) ∝
1
E(x, y)
(10)
The blue lines in Fig. 3 (a) and (b) show the re-
lationship between the input light intensity E and the
measurement I in the ordinary camera and the mea-
surement T in the proposed camera. While the mea-
surement I is proportional to the input E in the or-
dinary camera, the measurement T is nonlinear to the
(a) Exposure time image (b)Variable exposure image
Figure 4: Output of variable exposure camera: (a)Exposure
time image and (b)variable exposure image.
input E in the proposed camera. The red lines in Fig. 3
(a) and (b) show the resolution of measurements in
both cameras, that is
dI
dE
in the ordinary camera and
dT
dE
in the proposed camera. As shown in these im-
ages, the resolution of the proposed camera is large
for small input intensity, and is small for large input
intensity, while the resolution of the ordinary camera
is constant regardless of input intensity. This property
of the proposed camera enables us to capture small
difference in low input intensity avoiding the satura-
tion of high input intensity.
In the proposed method, the observedimage inten-
sity I(x, y) becomes constant I
θ
in an ideal case. How-
ever, it is actually not, since the exposure time is finite
and both the exposure time and the image intensity
have quantization errors. Therefore, we record both
the observed image intensity I(x, y) and the exposure
time T(x, y) simultaneously. From these recorded
informations, we can reconstruct HDR images effi-
ciently as we describe in the next section.
Fig. 4 shows an example output from the variable
exposure imaging. The left image shows exposure
time and the right image shows observed image in-
tensity which we call a variable exposure image. In
the exposure time image, the brightness of each pixel
shows the exposure time of the pixel. In the variable
exposure image, almost all pixels have similar inten-
sity to I
θ
, which indicates the exposure time for each
pixel is controlled appropriately. In addition, bright
area in exposure time image corresponds to dark area
in variable exposure image. It indicates that exposure
time becomes large, when the power of input light ray
is small.
3.2 HDR Image Reconstruction
We next consider the recovery of HDR images from
the exposure time image T(x, y) and the variable ex-
posure image I(x, y).
The HDR image reconstruction is equivalent to
the estimation of image E(x, y) obtained in a unit