View source for Single-sideband modulation

{{Modulation techniques}}
'''Single-sideband modulation''' ('''SSB''')  or ''Single-sideband suppressed-carrier'' (''SSB-SC'') is a refinement of [[amplitude modulation]] that more efficiently uses [[electric power|electrical power]] and [[bandwidth (signal processing)|bandwidth]]. 

[[Amplitude modulation]] produces a modulated output signal that has twice the bandwidth of the original [[baseband]] signal. Single-sideband modulation avoids this bandwidth doubling, and the power wasted on a carrier, at the cost of somewhat increased device complexity.

==History==
The first U.S. patent<ref>{{Patent|US|1449382|John Carson/AT&T: "Method and Means for Signaling with High Frequency Waves" filed on December 1, 1915; granted on March 27, 1923}}</ref> for SSB modulation was applied for on December 1, 1915 by [[John Renshaw Carson]]. The U.S. Navy experimented with SSB over its radio circuits before [[World War I]].<ref>[http://dj4br.home.t-link.de/ssb1e.htm The History of Single Sideband Modulation], ''Ing. Peter Weber''</ref><ref>[http://ieeexplore.ieee.org/xpl/freeabs_all.jsp?arnumber=4051940 IEEE, Early History of Single-Sideband Transmission,] ''Oswald, A.A.''</ref> SSB first entered commercial service on January 7, 1927 on the [[longwave]] transatlantic public radiotelephone circuit between New York and London.  The high power SSB transmitters were located at [[Rocky Point, New York]] and [[Rugby transmitting station|Rugby, England]].  The receivers were in very quiet locations in [[Houlton, Maine]] and [[Cupar]] Scotland.<ref>[http://massis.lcs.mit.edu/archives/history/underseas.cables History Of Undersea Cables], (1927)</ref>

SSB was also used over [[long distance calling|long distance]] [[telephone line]]s, as part of a technique known as [[frequency-division multiplexing]] (FDM). FDM was pioneered by telephone companies in the 1930s. This enabled many voice channels to be sent down a single physical circuit, for example in [[L-carrier]].  SSB allowed channels to be spaced (usually) just 4,000&nbsp;[[Hertz|Hz]] apart, while offering a speech bandwidth of nominally 300&ndash;3,400&nbsp;Hz.

[[Amateur radio operator]]s began serious experimentation with SSB after [[World War II]]. The [[Strategic Air Command]] established SSB as the radio standard for its aircraft in 1957.<ref>{{cite web|accessdate=
|format=PDF
|url=http://www.arrl.org/files/file/Technology/pdf/McElroy.pdf
|title=Amateur Radio and the Rise of SSB |publisher=National Association for Amateur Radio}}</ref> It has become a de facto standard for long-distance voice radio transmissions since then.

==Mathematical formulation==
SSB and vestigial side band (VSB) can also be regarded mathematically as special cases of analog [[quadrature amplitude modulation]].

Let <math>s(t)\,</math> be the [[baseband]] waveform to be transmitted.  Its [[Fourier transform]], <math>S(f)\,</math>, is [[Hermitian function|Hermitian symmetrical]] about the <math>f=0\,</math> axis, because <math>s(t)\,</math> is [[Real number|real-valued]].  [[Double sideband]] modulation of <math>s(t)\,</math> to a radio transmission frequency, <math>F_c\,</math>, moves the axis of symmetry to <math>f=\pm F_c</math>, and the two sides of each axis are called [[sidebands]].

Let <math>\widehat s(t)\,</math> represent the [[Hilbert transform]] of <math>s(t)\,</math>'''.''' &nbsp; Then

:<math>s_a(t) = s(t)+j\cdot \widehat s(t)\,</math>

is a useful mathematical concept, called an [[analytic signal]].  The Fourier transform of <math>s_a(t)\,</math> equals <math>2\cdot S(f)\,</math>, for <math>f > 0\,</math>, but it has no [[negative frequency|negative-frequency]] components.  So it can be modulated to a radio frequency and produce just a '''single''' sideband.

The analytic representation of <math>\cos(2\pi F_c\cdot t)\,</math> is''':'''

:<math>\cos(2\pi F_c\cdot t)+j\cdot \sin(2\pi F_c\cdot t) = e^{j2\pi F_c\cdot t}</math> &nbsp; (the equality is [[Euler's formula]])

whose Fourier transform is <math>\delta(f-F_c)\,</math>.

When <math>s_a(t)\,</math> is modulated (i.e. multiplied) by <math>e^{j2\pi F_c\cdot t}\,</math>, all frequency components are shifted by <math>+F_c\,</math>, so there are still no negative-frequency components.  Therefore, the complex product is an '''analytic representation''' of the single sideband signal''':'''

:<math>s_a(t)\cdot e^{j2\pi F_c\cdot t} = s_{ssb}(t) +j\cdot \widehat s_{ssb}(t) \,</math>

where <math>s_{ssb}(t)\,</math> is the real-valued, single sideband waveform.  Therefore''':'''

:{|
|-
|<math>s_{ssb}(t)\,</math>
|<math>= Re\big\{s_a(t)\cdot e^{j2\pi F_c\cdot t}\big\} </math>
|-
|
|<math>= Re\left\{\ [s(t)+j\cdot \widehat s(t)]\cdot [\cos(2\pi F_c\cdot t)+j\cdot \sin(2\pi F_c\cdot t)]\ \right\} </math>
|-
|
|<math>= s(t)\cdot \cos(2\pi F_c\cdot t) - \widehat s(t)\cdot \sin(2\pi F_c\cdot t)\,</math>
|}

The presence of two out-of-phase (quadrature) carrier waves is now evident.

===Lower sideband===
<math>s_a(t)\,</math> represents the baseband signal's [[upper sideband]], <math>s_{+}(t)\,</math>.  It is also possible, and useful, to convey the baseband information using its [[lower sideband]], <math>s_{-}(t)\,</math>, which is a mirror image about f=0&nbsp;Hz.  By a general property of the Fourier transform, that symmetry means it is the complex conjugate of <math>s_{+}(t)\,</math>''':'''

:<math>s_{-}(t) = s_{+}^*(t) = s_a^*(t) = s(t)-j\cdot \widehat s(t)\,</math>

Note that''':'''

:<math>s_{+}(t) + s_{-}(t) = 2s(t)\,</math>

The gain of 2 is a result of defining the analytic signal (one sideband) to have the same total energy as <math>s(t)\,</math> (both sidebands).

As before, the signal is modulated by <math>e^{j2\pi F_c\cdot t}\,</math>.  The typical <math>F_c\,</math> is large enough that the translated lower sideband (LSB) has no negative-frequency components.  Then the result is another analytic signal, whose real part is the actual transmission.

:{|
|-
|<math>s_{lsb}(t)\,</math>
|<math>= Re\big\{s_a^*(t)\cdot e^{j2\pi F_c\cdot t}\big\} </math>
|-
|
|<math>= s(t)\cdot \cos(2\pi F_c\cdot t) + \widehat s(t)\cdot \sin(2\pi F_c\cdot t)\,</math>
|}

Note that the sum of the two sideband signals is

:<math>2s(t)\cdot cos(2\pi F_c\cdot t)\,</math>

which is the classic model of suppressed-carrier [[double sideband]] AM.

==Practical implementations==
===Bandpass filtering===
[[File:SSB bandform.svg|thumb|The LSB spectrum is inverted compared to the baseband. As an example, a 2&nbsp;kHz audio baseband signal modulated onto a 5&nbsp;MHz carrier will produce a SSB frequency of 5.002000&nbsp;MHz if USB is used or 4.998000&nbsp;MHz if LSB is used.]]

A signal at frequency <math>f_0</math> amplitude-modulated onto a carrier wave at <math>f_m</math> can be expressed as simple multiplication of two cosine waves: <math>\cos(\omega_0t) \cos(\omega_mt) </math>, where <math>\omega_x = 2 \pi f_x</math>. Applying a simple trigonometric identity, we can change the above expression to be <math>\frac{1}{2} (\cos((\omega_m + \omega_0)t) + \cos((\omega_m - \omega_0)t))</math>. Each cosine term in the equation is known as a [[sideband]].

One method of producing an SSB signal is to remove one of the sidebands via [[Filter (signal processing)|filter]]ing, leaving only either the '''upper sideband''' ('''USB'''), the sideband with the higher frequency, or less commonly the '''lower sideband''' ('''LSB'''), the sideband with the lower frequency. Most often, the carrier is reduced or removed entirely (suppressed), being referred to in full as '''single sideband suppressed carrier''' ('''SSBSC'''). Assuming both sidebands are symmetric, which is the case for a normal [[Amplitude modulation|AM]] signal, no information is lost in the process.  Since the final RF amplification is now concentrated in a single sideband, the effective power output is greater than in normal AM (the carrier and redundant sideband account for well over half of the power output of an AM transmitter). Though SSB uses substantially less bandwidth and power, it cannot be demodulated by a simple [[envelope detector]] like standard AM.

===Hartley modulator===
An alternate method of generation known as a '''Hartley modulator''', named after [[Ralph Hartley|R. V. L. Hartley]], uses [[phase (waves)|phasing]] to suppress the unwanted sideband.  To generate an SSB signal with this method, two versions of the original signal are generated, mutually 90° out of phase for any single frequency within the operating bandwidth. Each one of these signals then modulates carrier waves (of one frequency) that are also 90° [[out of phase]] with each other. By either adding or subtracting the resulting signals, a lower or upper sideband signal results. A benefit of this approach is to allow an analytical expression for SSB signals, which can be used to understand effects such as synchronous detection of SSB.

Shifting the baseband signal 90° out of phase cannot be done simply by delaying it, as it contains a large range of frequencies. In analog circuits, a wideband 90-degree phase-difference network<ref>[http://home.earthlink.net/~christrask/pshift.html Earthlink.net], listing numerous articles.</ref> is used. The method was popular in the days of [[vacuum-tube]] radios, but later gained a bad reputation due to poorly adjusted commercial implementations.  Modulation using this method is again gaining popularity in the [[Amateur radio homebrew|homebrew]] and [[Digital signal processor|DSP]] fields.  This method, utilizing the [[Hilbert transform]] to phase shift the baseband audio, can be done at low cost with digital circuitry.

===Weaver modulator===
Another variation, the '''Weaver modulator''',<ref>"A Third Method of Generation and Detection of Single-Sideband Signals" D K Weaver Jr. Proc. IRE, Dec. 1956</ref> uses only lowpass filters and quadrature mixers, and is a favored method in digital implementations.

In Weaver's method, the band of interest is first translated to be centered at zero, conceptually by modulating a complex exponential <math>\exp(j\omega t)</math> with frequency in the middle of the voiceband, but implemented by a quadrature pair of sine and cosine modulators at that frequency (e.g. 2&nbsp;kHz).  This complex signal or pair of real signals is then lowpass filtered to remove the undesired sideband that is not centered at zero.  Then, the single-sideband complex signal centered at zero is upconverted to a real signal, by another pair of quadrature mixers, to the desired center frequency.

==Demodulation==
The front end of an SSB receiver is similar to that of an [[Amplitude_modulation|AM]] or [[Frequency modulation|FM]] receiver, consisting of a [[superheterodyne]] [[radio frequency|RF]] front end that produces a frequency-shifted version of the radio frequency (RF) signal within a standard [[intermediate frequency]] (IF) band. 

To recover the original signal from the IF SSB signal, the single sideband must be frequency-shifted down to its original range of [[baseband]] frequencies, by using a [[product detector]] which mixes it with the output of a [[beat frequency oscillator]] (BFO). In other words, it is just another stage of heterodyning.(mixing down to base band). For this to work, the BFO frequency must be exactly adjusted. 
If the BFO frequency is off, the output signal will be frequency-shifted (up or down), making speech sound strange and "[[Donald Duck]]"-like, or unintelligible. 
For audio communications, there is a common agreement about the BFO oscillator shift of 1.7kHz. A voice signal is sensitive to about 50Hz shift, with up to 100Hz still bearable. Some receivers use a [[carrier recovery]] system, which attempts to automatically lock on to the exact IF frequency. The carrier recovery doesn't solve the frequency shift. It gives better S/N ratio on the detector output.

As an example, consider an IF SSB signal centered at frequency <math>F_{if}\,</math> = 45000&nbsp;Hz. The baseband frequency it needs to be shifted to is <math>F_b\,</math> = 2000&nbsp;Hz. The BFO output waveform is <math>cos(2\pi\cdot F_{bfo}\cdot t)\,</math>. When the signal is multiplied by (aka '[[heterodyne]]d with') the BFO waveform, it shifts the signal to &nbsp;<math>(F_{if}+F_{bfo})\,</math> &nbsp;<u>and</u> to &nbsp;<math>|F_{if}-F_{bfo}|\,</math>, which is known as the ''beat frequency'' or ''image frequency''. The objective is to choose an <math>F_{bfo}\,</math> that results in &nbsp;<math>|F_{if}-F_{bfo}|=F_b\,</math> = 2000&nbsp;Hz. (The unwanted components at <math>(F_{if}+F_{bfo})\,</math> can be removed by a [[lowpass filter]] (for which an output transducer or the human [[ear]] may serve)).

Note that there are two choices for <math>F_{bfo}\,</math>''':''' 43000&nbsp;Hz and 47000&nbsp;Hz, a.k.a. ''low-side'' and ''high-side'' injection. With high-side injection, the spectral components that were distributed around 45000&nbsp;Hz will be distributed around 2000&nbsp;Hz in the reverse order, also known as an ''[[inverted spectrum]]''. That is in fact desirable when the IF spectrum is also inverted, because the BFO inversion restores the proper relationships. One reason for that is when the IF spectrum is the output of an inverting stage in the receiver. Another reason is when the SSB signal is actually a lower sideband, instead of an upper sideband. But if both reasons are true, then the IF spectrum in not inverted, and the non-inverting BFO (43000&nbsp;Hz) should be used.

If <math>F_{bfo}\,</math> is off by a small amount, then the beat frequency is not exactly <math>F_b\,</math>, which can lead to the speech distortion mentioned earlier.

== SSB as a speech-scrambling technique ==

SSB techniques can also be adapted to frequency-shift and frequency-invert baseband [[waveform]]s.
These effects were used, in conjunction with other filtering techniques, during [[World War II]] as a simple method for speech [[encryption]]. [[Radiotelephone]] [[conversation]]s between the US and [[United Kingdom|Britain]] were intercepted and "decrypted" by the Germans; they included some early conversations between [[Franklin D. Roosevelt]] and [[Winston Churchill|Churchill]].  In fact, the signals could be understood directly by trained operators.  Largely to allow secure communications between Roosevelt and Churchill, the [[SIGSALY]] system of digital encryption was devised.

Today, such simple inversion-based speech [[encryption]] techniques are easily decrypted using simple techniques and are no longer regarded as secure.

==Vestigial sideband (VSB)==
A '''vestigial sideband''' (in [[radio]] communication) is a [[sideband]] that has been only partly cut off or suppressed.  Television broadcasts (in analog video formats) use this method if the [[video]] is [[transmission (telecommunications)|transmitted]] in [[amplitude modulation|AM]], due to the large [[bandwidth (signal processing)|bandwidth]] used. It may also be used in digital transmission, such as the [[ATSC standard]]ized [[8-VSB]]. The Milgo 4400/48 [[modem]] (circa 1967) used vestigial sideband and [[phase-shift keying]] to provide 4800-bit/s transmission over a 1600&nbsp;Hz channel.

The video baseband signal used in TV in countries that use NTSC or ATSC has a bandwidth of 6&nbsp;MHz. To conserve bandwidth, SSB would be desirable, but the video signal has significant low frequency content (average brightness) and has rectangular synchronising pulses. The engineering compromise is vestigial sideband modulation. In vestigial sideband the full upper sideband of bandwidth W2 = 4&nbsp;MHz is transmitted, but only W1 = 1.25&nbsp;MHz of the lower sideband is transmitted, along with a carrier. This effectively makes the system AM at low modulation frequencies and SSB at high modulation frequencies. The absence of the lower sideband components at high frequencies must be compensated for, and this is done by the RF and IF filters.

==See also==
* [[ACSSB]],  amplitude-companded single sideband
* [[Independent sideband]]
* [[Modulation]] for other examples of modulation techniques
* [[Sideband]] for more general information about a sideband

==References==
<references/>

==General references==
*Partly from [[Federal Standard 1037C]] in support of [[MIL-STD-188]]

==Further reading==
* Sgrignoli, G., W. Bretl, R. and Citta. (1995). "VSB modulation used for terrestrial and cable broadcasts." ''IEEE Transactions on Consumer Electronics.'' v. 41, issue 3, p.&nbsp;367 - 382.
* J. Brittain, (1992). "Scanning the past: Ralph V.L. Hartley", ''Proc. IEEE'', vol.80,p.&nbsp;463.

{{Analogue TV transmitter topics}}

{{DEFAULTSORT:Single-Sideband Modulation}}
[[Category:Radio modulation modes]]
[[Category:Electronic design]]

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