Maximum length sequence

A maximum length sequence (MLS) is a type of pseudorandom binary sequence.

They are bit sequences generated using maximal linear feedback shift registers and are so called because they are periodic and reproduce every binary sequence (except the zero vector) that can be represented by the shift registers (i.e., for length-m registers they produce a sequence of length 2^m − 1). An MLS is also sometimes called an n-sequence or an m-sequence. MLSs are spectrally flat, with the exception of a near-zero DC term.

These sequences may be represented as coefficients of irreducible polynomials in a polynomial ring over Z/2Z.

Practical applications for MLS include measuring impulse responses (e.g., of room reverberation). They are also used as a basis for deriving pseudo-random sequences in digital communication systems that employ direct-sequence spread spectrum and frequency-hopping spread spectrum transmission systems, optical dielectric multilayer reflector design,[1] and in the efficient design of some fMRI experiments.[2]

Generation

Figure 1: The next value of register a₃ in a feedback shift register of length 4 is determined by the modulo-2 sum of a₀ and a₁.

MLS are generated using maximal linear feedback shift registers. An MLS-generating system with a shift register of length 4 is shown in Fig. 1. It can be expressed using the following recursive relation:

${\displaystyle {\begin{cases}a_{3}[n+1]=a_{0}[n]+a_{1}[n]\\a_{2}[n+1]=a_{3}[n]\\a_{1}[n+1]=a_{2}[n]\\a_{0}[n+1]=a_{1}[n]\\\end{cases}}}$

where n is the time index and ${\displaystyle +}$ represents modulo-2 addition. For bit values 0 = FALSE or 1 = TRUE, this is equivalent to the XOR operation.

As MLS are periodic and shift registers cycle through every possible binary value (with the exception of the zero vector), registers can be initialized to any state, with the exception of the zero vector.

Polynomial interpretation

A polynomial over GF(2) can be associated with the linear feedback shift register. It has degree of the length of the shift register, and has coefficients that are either 0 or 1, corresponding to the taps of the register that feed the xor gate. For example, the polynomial corresponding to Figure 1 is x⁴ + x¹ + 1.

A necessary and sufficient condition for the sequence generated by a LFSR to be maximal length is that its corresponding polynomial be primitive.[3]

Implementation

MLS are inexpensive to implement in hardware or software, and relatively low-order feedback shift registers can generate long sequences; a sequence generated using a shift register of length 20 is 2²⁰ − 1 samples long (1,048,575 samples).

Properties of maximum length sequences

MLS have the following properties, as formulated by Solomon Golomb.[4]

Balance property

The occurrence of 0 and 1 in the sequence should be approximately the same. More precisely, in a maximum length sequence of length ${\displaystyle 2^{n}-1}$ there are ${\displaystyle 2^{n-1}}$ ones and ${\displaystyle 2^{n-1}-1}$ zeros. The number of ones equals the number of zeros plus one, since the state containing only zeros cannot occur.

Run property

A "run" is a sub-sequence of consecutive "1"s or consecutive "0"s within the MLS concerned. The number of runs is the number of such sub-sequences.

Of all the "runs" (consisting of "1"s or "0"s) in the sequence :

• One half of the runs are of length 1.
• One quarter of the runs are of length 2.
• One eighth of the runs are of length 3.
• ... etc. ...

Correlation property

The circular autocorrelation of an MLS is a Kronecker delta function[5][6] (with DC offset and time delay, depending on implementation). For the ±1 convention, i.e., bit value 1 is assigned ${\displaystyle s=+1}$ and bit value 0 ${\displaystyle s=-1}$, mapping XOR to the negative of the product:

${\displaystyle R(n)={\frac {1}{N}}\sum _{m=1}^{N}s[m]\,s^{*}[m+n]_{N}={\begin{cases}1&{\text{if }}n=0,\\-{\frac {1}{N}}&{\text{if }}0<n<N.\end{cases}}}$

where ${\displaystyle s^{*}}$ represents the complex conjugate and ${\displaystyle [m+n]_{N}}$ represents a circular shift.

The linear autocorrelation of an MLS approximates a Kronecker delta.

Extraction of impulse responses

If a linear time invariant (LTI) system's impulse response is to be measured using a MLS, the response can be extracted from the measured system output y[n] by taking its circular cross-correlation with the MLS. This is because the autocorrelation of a MLS is 1 for zero-lag, and nearly zero (−1/N where N is the sequence length) for all other lags; in other words, the autocorrelation of the MLS can be said to approach unit impulse function as MLS length increases.

If the impulse response of a system is h[n] and the MLS is s[n], then

${\displaystyle y[n]=(h*s)[n].\,}$

Taking the cross-correlation with respect to s[n] of both sides,

${\displaystyle {\phi }_{sy}=h[n]*{\phi }_{ss}\,}$

and assuming that φ_ss is an impulse (valid for long sequences)

${\displaystyle h[n]={\phi }_{sy}.\,}$

Any signal with an impulsive autocorrelation can be used for this purpose, but signals with high crest factor, such as the impulse itself, produce impulse responses with poor signal-to-noise ratio. It's commonly assumed that the MLS would then be the ideal signal, as it consists of only full-scale values and its digital crest factor is the minimum, 0 dB.[7][8] However, after analog reconstruction, the sharp discontinuities in the signal produce strong intersample peaks, degrading the crest factor by 4-8 dB or more, increasing with signal length, making it worse than a sine sweep.[9] Other signals have been designed with minimal crest factor, though it's unknown if it can be improved beyond 3 dB.[10]

Relationship to Hadamard transform

Cohn and Lempel[11] showed the relationship of the MLS to the Hadamard transform. This relationship allows the correlation of an MLS to be computed in a fast algorithm similar to the FFT.

See also

• Barker code
• Complementary sequences
• Federal Standard 1037C
• Frequency response
• Gold code
• Impulse response
• Polynomial ring

References

• Golomb, Solomon W.; Guang Gong (2005). Signal Design for Good Correlation: For Wireless Communication, Cryptography, and Radar. Cambridge University Press. ISBN 978-0-521-82104-9.

1. Poudel, Khem Narayan; Robertson, William M. (2018-10-15). "Maximum length sequence dielectric multilayer reflector". OSA Continuum. 1 (2): 358–372. doi:10.1364/OSAC.1.000358. ISSN 2578-7519.
2. Buracas GT, Boynton GM (July 2002). "Efficient design of event-related fMRI experiments using M-sequences". NeuroImage. 16 (3 Pt 1): 801–13. doi:10.1006/nimg.2002.1116. PMID 12169264.
3. "Linear Feedback Shift Registers- Implementation, M-Sequence Properties, Feedback Tables", New Wave Instruments (NW), Retrieved 2013.12.03.
4. Golomb, Solomon W. (1967). Shift register sequences. Holden-Day. ISBN 0-89412-048-4.
5. Jacobsen, Finn; Juhl, Peter Moller (2013-06-04). Fundamentals of General Linear Acoustics. John Wiley & Sons. ISBN 978-1118636176. A maximum-length sequence is a binary sequence whose circular autocorrelation (except for a small DC-error) is a delta function.
6. Sarwate, D. V.; Pursley, M. B. (1980-05-01). "Crosscorrelation properties of pseudorandom and related sequences". Proceedings of the IEEE. 68 (5): 593–619. doi:10.1109/PROC.1980.11697. ISSN 0018-9219.
7. "A Little MLS (Maximum-Length Sequence) Tutorial | dspGuru.com". dspguru.com. Retrieved 2016-05-19. its RMS and peak values are both X, making its crest factor (peak/RMS) equal to 1, the lowest it can get.
8. "Other Electro-Acoustical Measurement Techniques". www.clear.rice.edu. Retrieved 2016-05-19. The crest factor for MLS is very close to 1, so it makes sense to use this kind of input signal when we need a high signal-to-noise ratio for our measurement
9. Chan, Ian H. "Swept Sine Chirps for Measuring Impulse Response" (PDF). thinksrs.com. Retrieved 2016-05-19.
10. Friese, M. (1997-10-01). "Multitone signals with low crest factor" (PDF). IEEE Transactions on Communications. 45 (10): 1338–1344. doi:10.1109/26.634697. ISSN 0090-6778.
11. Cohn, M.; Lempel, A. (January 1977). "On Fast M-Sequence Transforms". IEEE Trans. Inf. Theory. 23 (1): 135–7. doi:10.1109/TIT.1977.1055666.

External links

• Bristow-Johnson, Robert. "A Little MLS Tutorial". — Short on-line tutorial describing how MLS is used to obtain the impulse response of a linear time-invariant system. Also describes how nonlinearities in the system can show up as spurious spikes in the apparent impulse response.
• Hee, Jens. "Impulse response measurement using MLS" (PDF). — Paper describing MLS generation. Contains C-code for MLS generation using up to 18-tap-LFSRs and matching Hadamard transform for impulse response extraction.
• Kerr, Wesley; Drucker, Daniel. "Creation of M-Sequences". Geoffrey Aguirre Lab. University of Pennsylvania.
• "Linear Feedback Shift Registers". New Wave Instruments. 2005. — Properties of maximal length sequences, and comprehensive feedback tables for maximal lengths from 7 to 16,777,215 (3 to 24 stages), and partial tables for lengths up to 4,294,967,295 (25 to 32 stages).
• Schäfer, Magnus (October 2012). "Aachen Impulse Response Database". Institute of Communication Systems and Data Processing, RWTH Aachen University. V1.4. A (binaural) room impulse response database generated by means of maximum length sequences]
• "Efficient Shift Registers, LFSR Counters, and Long Pseudo-Random Sequence Generators — Obsolete" (PDF). Xilinx. July 1996. XAPP052 v1.1. — Implementing lfsr's in FPGAs includes listing of taps for 3 to 168 bits