(communications) Division of the range of values of a wave into a finite number of subranges, each of which is represented by an assigned or quantized value within the subrange.
(quantum mechanics) The restriction of an observable quantity, such as energy or angular momentum, associated with a physical system, such as an atom, molecule, or elementary particle, to a discrete set of values. The transition from a description of a system of particles or fields in the classical approximation where canonically conjugate variables commute, to a description where these variables are treated as noncommuting operators; quantization (first definition) is a result of this procedure.
(science and technology) The restriction of a variable to a discrete number of possible values; thus the age of a person is usually quantized as a whole number of years.
(1) The division of a range of values into a single number, code or classification. For example, class A is 0 to 999, class B is 1000 to 9999 and class C is 10000 and above.
(2) In analog to digital conversion, the assignment of a number to the amplitude of a wave. The larger the range of numbers, the finer the increments can be measured, and the more the digital sample represents the analog signal. See sampling and quantization error.
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Quantization, in mathematics and digital signal processing, is the process of mapping a large set of input values to a smaller set – such as rounding values to some unit of precision. A device or algorithmic function that performs quantization is called a quantizer. The error introduced by quantization is referred to as quantization error or round-off error. Quantization is involved to some degree in nearly all digital signal processing, as the process of representing a signal in digital form ordinarily involves rounding. Quantization also forms the core of essentially all lossy compression algorithms.
Because quantization is a many-to-few mapping, it is an inherently non-linear and irreversible process (i.e., because the same output value is shared by multiple input values, it is impossible in general to recover the exact input value when given only the output value).
The set of possible input values may be infinitely large, and may possibly be continuous and therefore uncountable (such as the set of all real numbers, or all real numbers within some limited range). The set of possible output values may be finite or countably infinite. The input and output sets involved in quantization can be defined in a rather general way. For example, vector quantization is the application of quantization to multi-dimensional (vector-valued) input data.[1]
There are two substantially different classes of applications where quantization is used:
The analysis of quantization involves studying the amount of data (typically measured in digits or bits or bit rate) that is used to represent the output of the quantizer, and studying the loss of precision that is introduced by the quantization process (which is referred to as the distortion). The general field of such study of rate and distortion is known as rate–distortion theory.
The most common type of quantization is known as scalar quantization. Scalar quantization, typically denoted as
, is the process of using a quantization function
( ) to map a scalar (one-dimensional) input value
to a scalar output value
. Scalar quantization can be as simple and intuitive as rounding high-precision numbers to the nearest integer, or to the nearest multiple of some other unit of precision (such as rounding a large monetary amount to the nearest thousand dollars). Scalar quantization of continuous-valued input data that is performed by an electronic sensor is referred to as analog-to-digital conversion. Analog-to-digital conversion often also involves sampling the signal periodically in time (e.g., at 44.1 kHz for CD-quality audio signals).
As an example, rounding a real number
to the nearest integer value forms a very basic type of quantizer – a uniform one. A typical (mid-tread) uniform quantizer with a quantization step size equal to some value
can be expressed as
,
where the function
( ) is the sign function (also known as the signum function). For simple rounding to the nearest integer, the step size
is equal to 1. With
or with
equal to any other integer value, this quantizer has real-valued inputs and integer-valued outputs, although this property is not a necessity – a quantizer may also have an integer input domain and may also have non-integer output values. The essential property of a quantizer is that it has a countable set of possible output values that has fewer members than the set of possible input values. The members of the set of output values may have integer, rational, or real values (or even other possible values as well, in general – such as vector values or complex numbers).
When the quantization step size is small (relative to the variation in the signal being measured), it is relatively simple to show[2][3][4][5][6][7] that the mean squared error produced by such a rounding operation will be approximately
.
Because the set of possible output values of a quantizer is countable, any quantizer can be decomposed into two distinct stages, which can be referred to as the classification stage (or forward quantization stage) and the reconstruction stage (or inverse quantization stage), where the classification stage maps the input value to an integer quantization index
and the reconstruction stage maps the index
to the reconstruction value
that is the output approximation of the input value. For the example uniform quantizer described above, the forward quantization stage can be expressed as
,
and the reconstruction stage for this example quantizer is simply
.
This decomposition is useful for the design and analysis of quantization behavior, and it illustrates how the quantized data can be communicated over a communication channel – a source encoder can perform the forward quantization stage and send the index information through a communication channel (possibly applying entropy coding techniques to the quantization indices), and a decoder can perform the reconstruction stage to produce the output approximation of the original input data. In more elaborate quantization designs, both the forward and inverse quantization stages may be substantially more complex. In general, the forward quantization stage may use any function that maps the input data to the integer space of the quantization index data, and the inverse quantization stage can conceptually (or literally) be a table look-up operation to map each quantization index to a corresponding reconstruction value. This two-stage decomposition applies equally well to vector as well as scalar quantizers.
Most uniform quantizers for signed input data can be classified as being of one of two types: mid-riser and mid-tread. The terminology is based on what happens in the region around the value 0, and uses the analogy of viewing the input-output function of the quantizer as a stairway. Mid-tread quantizers have a zero-valued reconstruction level (corresponding to a tread of a stairway), while mid-riser quantizers have a zero-valued classification threshold (corresponding to a riser of a stairway).[8]
The formulas for mid-tread uniform quantization are provided above.
The input-output formula for a mid-riser uniform quantizer is given by:
,
where the classification rule is given by
and the reconstruction rule is
.
Note that mid-riser uniform quantizers do not have a zero output value – their minimum output magnitude is half the step size. When the input data can be modeled as a random variable with a probability density function (pdf) that is smooth and symmetric around zero, mid-riser quantizers also always produce an output entropy of at least 1 bit per sample.
In contrast, mid-tread quantizers do have a zero output level, and can reach arbitrarily low bit rates per sample for input distributions that are symmetric and taper off at higher magnitudes. For some applications, having a zero output signal representation or supporting low output entropy may be a necessity. In such cases, using a mid-tread uniform quantizer may be appropriate while using a mid-riser one would not be.
In general, a mid-riser or mid-tread quantizer may not actually be a uniform quantizer – i.e., the size of the quantizer's classification intervals may not all be the same, or the spacing between its possible output values may not all be the same. The distinguishing characteristic of a mid-riser quantizer is that it has a classification threshold value that is exactly zero, and the distinguishing characteristic of a mid-tread quantizer is that is it has a reconstruction value that is exactly zero.[8]
Another name for a mid-tread quantizer is dead-zone quantizer, and the classification region around the zero output value of such a quantizer is referred to as the dead zone. The dead zone can sometimes serve the same purpose as a noise gate or squelch function.
Often the design of a quantizer involves supporting only a limited range of possible output values and performing clipping to limit the output to this range whenever the input exceeds the supported range. The error introduced by this clipping is referred to as overload distortion. Within the extreme limits of the supported range, the amount of spacing between the selectable output values of a quantizer is referred to as its granularity, and the error introduced by this spacing is referred to as granular distortion. It is common for the design of a quantizer to involve determining the proper balance between granular distortion and overload distortion. For a given supported number of possible output values, reducing the average granular distortion may involve increasing the average overload distortion, and vice-versa. A technique for controlling the amplitude of the signal (or, equivalently, the quantization step size
) to achieve the appropriate balance is the use of automatic gain control (AGC). However, in some quantizer designs, the concepts of granular error and overload error may not apply (e.g., for a quantizer with a limited range of input data or with a countably infinite set of selectable output values).
A common assumption for the analysis of quantization error is that it affects a signal processing system in a similar manner to that of additive white noise – having negligible correlation with the signal and an approximately flat power spectral density.[3][9][10][7] The additive noise model is commonly used for the analysis of quantization error effects in digital filtering systems, and it can be very useful in such analysis. It has been shown to be a valid model in cases of high resolution quantization (small
relative to the signal strength) with smooth probability density functions.[3][11] However, additive noise behaviour is not always a valid assumption, and care should be taken to avoid assuming that this model always applies. In actuality, the quantization error (for quantizers defined as described here) is deterministically related to the signal rather than being independent of it,[7] and in some cases it can even cause limit cycles to appear in digital signal processing systems.[10]
One way to ensure effective independence of the quantization error from the source signal is to perform dithered quantization (sometimes with noise shaping), which involves adding random (or pseudo-random) noise to the signal prior to quantization.[10][7] This can sometimes be beneficial for such purposes as improving the subjective quality of the result, however it can increase the total quantity of error introduced by the quantization process.
A scalar quantizer, which performs a quantization operation, can ordinarily be decomposed into two stages:
non-overlapping intervals
, by defining
boundary (decision) values
, such that
for
, with the extreme limits defined by
and
. All the inputs
that fall in a given interval range
are associated with the same quantization index
.
is represented by a reconstruction value
which implements the mapping
.These two stages together comprise the mathematical operation of
.
Entropy coding techniques can be applied to communicate the quantization indices from a source encoder that performs the classification stage to a decoder that performs the reconstruction stage. One way to do this is to associate each quantization index
with a binary codeword
. An important consideration is the number of bits used for each codeword, denoted here by
.
As a result, the design of an
-level quantizer and an associated set of codewords for communicating its index values requires finding the values of
,
and
which optimally satisfy a selected set of design constraints such as the bit rate
and distortion
.
Assuming that an information source
produces random variables
with an associated probability density function
, the probability
that the random variable falls within a particular quantization interval
is given by
.
The resulting bit rate
, in units of average bits per quantized value, for this quantizer can be derived as follows:
.
If it is assumed that distortion is measured by mean squared error, the distortion D, is given by:
.
Note that other distortion measures can also be considered, although mean squared error is a popular one.
A key observation is that rate
depends on the decision boundaries
and the codeword lengths
, whereas the distortion
depends on the decision boundaries
and the reconstruction levels
.
After defining these two performance metrics for the quantizer, a typical Rate–Distortion formulation for a quantizer design problem can be expressed in one of two ways:
, minimize the bit rate 
, minimize the distortion 
Often the solution to these problems can be equivalently (or approximately) expressed and solved by converting the formulation to the unconstrained problem
where the Lagrange multiplier
is a non-negative constant that establishes the appropriate balance between rate and distortion. Solving the unconstrained problem is equivalent to finding a point on the convex hull of the family of solutions to an equivalent constrained formulation of the problem. However, finding a solution – especially a closed-form solution – to any of these three problem formulations can be difficult. Solutions that do not require multi-dimensional iterative optimization techniques have been published for only three probability distribution functions: the uniform,[12] exponential,[13] and Laplacian[13] distributions. Iterative optimization approaches can be used to find solutions in other cases.[14][15][7]
Note that the reconstruction values
affect only the distortion – they do not affect the bit rate – and that each individual
makes a separate contribution
to the total distortion as shown below:
where
This observation can be used to ease the analysis – given the set of
values, the value of each
can be optimized separately to minimize its contribution to the distortion
.
For the mean-square error distortion criterion, it can be easily shown that the optimal set of reconstruction values
is given by setting the reconstruction value
within each interval
to the conditional expected value (also referred to as the centroid) within the interval, as given by:
.
The use of sufficiently well-designed entropy coding techniques can result in the use of a bit rate that is close to the true information content of the indices
, such that effectively
and therefore
The use of this approximation can allow the entropy coding design problem to be separated from the design of the quantizer itself. Modern entropy coding techniques such as arithmetic coding can achieve bit rates that are very close to the true entropy of a source, given a set of known (or adaptively estimated) probabilities
.
In some designs, rather than optimizing for a particular number of classification regions
, the quantizer design problem may include optimization of the value of
as well. For some probabilistic source models, the best performance may be achieved when
approaches infinity.
In the above formulation, if the bit rate constraint is neglected by setting
equal to 0, or equivalently if it is assumed that a fixed-length code (FLC) will be used to represent the quantized data instead of a variable-length code (or some other entropy coding technology such as arithmetic coding that is better than an FLC in the rate–distortion sense), the optimization problem reduces to minimization of distortion
alone.
The indices produced by an
-level quantizer can be coded using a fixed-length code using
bits/symbol. For example when
256 levels, the FLC bit rate
is 8 bits/symbol. For this reason, such a quantizer has sometimes been called an 8-bit quantizer. However using an FLC eliminates the compression improvement that can be obtained by use of better entropy coding.
Assuming an FLC with
levels, the Rate–Distortion minimization problem can be reduced to distortion minimization alone. The reduced problem can be stated as follows: given a source
with pdf
and the constraint that the quantizer must use only
classification regions, find the decision boundaries
and reconstruction levels
to minimize the resulting distortion
Finding an optimal solution to the above problem results in a quantizer sometimes called a MMSQE (minimum mean-square quantization error) solution, and the resulting pdf-optimized (non-uniform) quantizer is referred to as a Lloyd–Max quantizer, named after two people who independently developed iterative methods[16][17][7] to solve the two sets of simultaneous equations resulting from
and
, as follows:
,
which places each threshold at the mid-point between each pair of reconstruction values, and
which places each reconstruction value at the centroid (conditional expected value) of its associated classification interval.
Lloyd's Method I algorithm, originally described in 1957, can be generalized in a straighforward way for application to vector data. This generalization results in the Linde–Buzo–Gray (LBG) or k-means classifier optimization methods. Moreover, the technique can be further generalized in a straightforward way to also include an entropy constraint for vector data.[18]
The Lloyd–Max quantizer is actually a uniform quantizer when the input pdf is uniformly distributed over the range
. However, for a source that does not have a uniform distribution, the minimum-distortion quantizer may not be a uniform quantizer.
The analysis of a uniform quantizer applied to a uniformly distributed source can be summarized in what follows:
A symmetric source X can be modelled with
, for
and 0 elsewhere. The step size
and the signal to quantization noise ratio (SQNR) of the quantizer is
SQNR
.
For a fixed-length code using
bits,
, resulting in
SQNR
dB,
or approximately 6 dB per bit. For example, for
=8 bits,
=256 levels and SQNR = 8*6 = 48 dB; and for
=16 bits,
=65536 and SQNR = 16*6 = 96 dB. The property of 6 dB improvement in SQNR for each extra bit used in quantization is a well-known figure of merit. However, it must be used with care: this derivation is only for a uniform quantizer applied to a uniform source.
For other source pdfs and other quantizer designs, the SQNR may be somewhat different than predicted by 6 dB/bit, depending on the type of pdf, the type of source, the type of quantizer, and the bit rate range of operation.
However, it is common to assume that for many sources, the slope of a quantizer SQNR function can be approximated as 6 dB/bit when operating at a sufficiently high bit rate. At asymptotically high bit rates, cutting the step size in half increases the bit rate by approximately 1 bit per sample (because 1 bit is needed to indicate whether the value is in the left or right half of the prior double-sized interval) and reduces the mean squared error by a factor of 4 (i.e., 6 dB) based on the
approximation.
At asymptotically high bit rates, the 6 dB/bit approximation is supported for many source pdfs by rigorous theoretical analysis.[3][4][6][7] Moreover, the structure of the optimal scalar quantizer (in the rate–distortion sense) approaches that of a uniform quantizer under these conditions.[6][7]
Companded quantization is the combination of three functional building blocks – namely, a (continuous-domain) signal dynamic range compressor, a limited-range uniform quantizer, and a (continuous-domain) signal dynamic range expander that basically inverts the compressor function. This type of quantization is frequently used in older speech telephony systems. The compander function of the compressor is key to the performance of such a quantization system. In principle, the compressor function can be designed to exactly map the boundaries of the optimal intervals of any desired scalar quantizer function to the equal-size intervals used by the uniform quantizer and similarly the expander function can exactly map the uniform quantizer reconstruction values to any arbitrary reconstruction values. Thus, with arbitrary compressor and expander functions, any possible non-uniform scalar quantizer can be equivalently implemented as a companded quantizer.[3][7] In practice, companders are designed to operate according to relatively simple dynamic range compressor functions that are designed to be suitable for implementation using simple analog electronic circuits. The two most popular compander functions used for telecommunications are the A-law and μ-law functions.
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