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Quadrature amplitude modulation
Quadrature amplitude modulation
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Quadrature amplitude modulation (QAM) is the name of a family of digital modulation methods and a related family of analog modulation methods widely used in modern telecommunications to transmit information. It conveys two analog message signals, or two digital bit streams, by changing (modulating) the amplitudes of two carrier waves, using the amplitude-shift keying (ASK) digital modulation scheme or amplitude modulation (AM) analog modulation scheme. The two carrier waves are of the same frequency and are out of phase with each other by 90°, a condition known as orthogonality or quadrature. The transmitted signal is created by adding the two carrier waves together. At the receiver, the two waves can be coherently separated (demodulated) because of their orthogonality. Another key property is that the modulations are low-frequency/low-bandwidth waveforms compared to the carrier frequency, which is known as the narrowband assumption.

Phase modulation (analog PM) and phase-shift keying (digital PSK) can be regarded as a special case of QAM, where the amplitude of the transmitted signal is a constant, but its phase varies. This can also be extended to frequency modulation (FM) and frequency-shift keying (FSK), for these can be regarded as a special case of phase modulation. [citation needed]

QAM is used extensively as a modulation scheme for digital communications systems, such as in 802.11 Wi-Fi standards. Arbitrarily high spectral efficiencies can be achieved with QAM by setting a suitable constellation size, limited only by the noise level and linearity of the communications channel.[1]  QAM is being used in optical fiber systems as bit rates increase; QAM16 and QAM64 can be optically emulated with a three-path interferometer.[2][3]

Demodulation

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Analog QAM: PAL color bar signal on a vectorscope

In a QAM signal, one carrier lags the other by 90°, and its amplitude modulation is customarily referred to as the in-phase component, denoted by I(t). The other modulating function is the quadrature component, Q(t). So the composite waveform is mathematically modeled as:

    or:

where fc is the carrier frequency.  At the receiver, a coherent demodulator multiplies the received signal separately with both a cosine and sine signal to produce the received estimates of I(t) and Q(t). For example:

Using standard trigonometric identities, we can write this as:

Low-pass filtering r(t) removes the high frequency terms (containing fct), leaving only the I(t) term. This filtered signal is unaffected by Q(t), showing that the in-phase component can be received independently of the quadrature component.  Similarly, we can multiply sc(t) by a sine wave and then low-pass filter to extract Q(t).

The graphs of the sine (solid red) and cosine (dotted blue) functions are sinusoids of different phases.

The addition of two sinusoids is a linear operation that creates no new frequency components. So the bandwidth of the composite signal is comparable to the bandwidth of the DSB (double-sideband) components. Effectively, the spectral redundancy of DSB enables a doubling of the information capacity using this technique. This comes at the expense of demodulation complexity. In particular, a DSB signal has zero-crossings at a regular frequency, which makes it easy to recover the phase of the carrier sinusoid. It is said to be self-clocking. But the sender and receiver of a quadrature-modulated signal must share a clock or otherwise send a clock signal. If the clock phases drift apart, the demodulated I and Q signals bleed into each other, yielding crosstalk. In this context, the clock signal is called a "phase reference". Clock synchronization is typically achieved by transmitting a burst subcarrier or a pilot signal. The phase reference for NTSC, for example, is included within its colorburst signal.

Analog QAM is used in:

  • NTSC and PAL analog color television systems, where the I- and Q-signals carry the components of chroma (colour) information. The QAM carrier phase is recovered from a special colorburst transmitted at the beginning of each scan line.
  • C-QUAM ("Compatible QAM") is used in AM stereo radio to carry the stereo difference information.

Fourier analysis

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Applying Euler's formula to the sinusoids in Eq.1, the positive-frequency portion of sc (or analytic representation) is:

where denotes the Fourier transform, and ︿I and ︿Q are the transforms of I(t) and Q(t). This result represents the sum of two DSB-SC signals with the same center frequency. The factor of i (= e/2) represents the 90° phase shift that enables their individual demodulations.

Digital QAM

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Digital 16-QAM with example symbols
Digital 16-QAM with example symbols
Constellation points for 4-QAM, 16-QAM, 32-QAM, and 64-QAM overlapped

As in many digital modulation schemes, the constellation diagram is useful for QAM. In QAM, the constellation points are usually arranged in a square grid with equal vertical and horizontal spacing, although other configurations are possible (e.g. a hexagonal or triangular grid). In digital telecommunications the data is usually binary, so the number of points in the grid is typically a power of 2 (2, 4, 8, …), corresponding to the number of bits per symbol. The simplest and most commonly used QAM constellations consist of points arranged in a square, i.e. 16-QAM, 64-QAM and 256-QAM (even powers of two). Non-square constellations, such as Cross-QAM, can offer greater efficiency but are rarely used because of the cost of increased modem complexity.

By moving to a higher-order constellation, it is possible to transmit more bits per symbol. However, if the mean energy of the constellation is to remain the same (by way of making a fair comparison), the points must be closer together and are thus more susceptible to noise and other corruption; this results in a higher bit error rate and so higher-order QAM can deliver more data less reliably than lower-order QAM, for constant mean constellation energy. Using higher-order QAM without increasing the bit error rate requires a higher signal-to-noise ratio (SNR) by increasing signal energy, reducing noise, or both.

If data rates beyond those offered by 8-PSK are required, it is more usual to move to QAM since it achieves a greater distance between adjacent points in the I-Q plane by distributing the points more evenly. The complicating factor is that the points are no longer all the same amplitude and so the demodulator must now correctly detect both phase and amplitude, rather than just phase.

64-QAM and 256-QAM are often used in digital cable television and cable modem applications. In the United States, 64-QAM and 256-QAM are the mandated modulation schemes for digital cable (see QAM tuner) as standardised by the SCTE in the standard ANSI/SCTE 07 2013. In the UK, 64-QAM is used for digital terrestrial television (Freeview) whilst 256-QAM is used for Freeview-HD.

Bit-loading (bits per QAM constellation) on an ADSL line

Communication systems designed to achieve very high levels of spectral efficiency usually employ very dense QAM constellations. For example is ADSL technology for copper twisted pairs, whose constellation size goes up to 32768-QAM (in ADSL terminology this is referred to as bit-loading, or bit per tone, 32768-QAM being equivalent to 15 bits per tone).[4]

Ultra-high capacity microwave backhaul systems also use 1024-QAM.[5] With 1024-QAM, adaptive coding and modulation (ACM) and XPIC, vendors can obtain gigabit capacity in a single 56 MHz channel.[5]

Interference and noise

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In moving to a higher order QAM constellation (higher data rate and mode) in hostile RF/microwave QAM application environments, such as in broadcasting or telecommunications, multipath interference typically increases. There is a spreading of the spots in the constellation, decreasing the separation between adjacent states, making it difficult for the receiver to decode the signal appropriately. In other words, there is reduced noise immunity. There are several test parameter measurements which help determine an optimal QAM mode for a specific operating environment. The following three are most significant:[6]

See also

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References

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Further reading

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Revisions and contributorsEdit on WikipediaRead on Wikipedia
from Grokipedia
Quadrature amplitude modulation (QAM) is a modulation technique that transmits data by modulating the of two carrier signals of the same but differing in phase by 90 degrees, known as in-phase (I) and quadrature (Q) components. These two signals are combined to form a single composite signal, allowing the efficient encoding of information in both and phase variations. At the receiver, the signals are separated using quadrature to recover the original data. QAM generalizes (PAM) for bandpass channels by representing the transmitted signal as a complex envelope, where the real part corresponds to the I-channel and the imaginary part to the Q-channel. This approach achieves twice the bandwidth efficiency of single-carrier PAM since the two orthogonal carriers do not interfere. The possible signal states are depicted in a two-dimensional signal constellation diagram, where each point represents a unique combination of I and Q amplitudes, enabling higher-order modulations such as 16-QAM or 256-QAM for increased data rates. Linear channel distortions in QAM systems can be mitigated through adaptive equalization. QAM is widely applied in modern telecommunications due to its spectral efficiency and robustness in noisy environments when combined with error-correcting codes. Common uses include digital subscriber lines (DSL), cable modems, Wi-Fi networks, high-definition television (HDTV) broadcasting, and 4G/5G mobile communications. Higher-order QAM variants, such as 64-QAM and 256-QAM, support greater throughput but require higher signal-to-noise ratios to maintain reliability.

Fundamentals

Definition and Principles

Quadrature amplitude modulation (QAM) is a modulation technique that encodes information by varying the s of two carrier signals of the same but differing in phase by 90 degrees, typically a cosine wave and a . These carriers are independently modulated in by separate message signals and then combined into a single transmitted . To understand QAM, it is helpful to first consider (AM), a foundational in which the of a high-frequency carrier signal is systematically varied according to the instantaneous value of a lower-frequency message signal, while the carrier's and phase remain constant. In QAM, the in-phase (I) component modulates the cosine carrier, and the quadrature (Q) component modulates the sine carrier; these are added together to produce the modulated signal. The 90-degree phase shift ensures between the I and Q carriers, meaning their inner product over a complete cycle is zero, which prevents interference between the two modulated signals during transmission. This orthogonal structure provides key advantages over single-carrier AM methods, including greater , as QAM transmits two independent signals within the bandwidth required for one, effectively doubling the data rate for the same channel bandwidth. The approach is particularly valuable in bandwidth-constrained environments, such as radio communications, where maximizing information throughput without expanding spectrum usage is essential. A basic QAM transmitter block diagram includes two amplitude modulators: one multiplies the I message signal with the cosine carrier, while the other multiplies the Q message signal with the phase-shifted sine carrier; the outputs are then summed to form the composite signal for transmission. At the receiver, the incoming signal is split and multiplied by locally generated cosine and sine carriers from a synchronized oscillator, followed by low-pass filters to recover the original I and Q components separately, exploiting the orthogonality to eliminate cross-talk.

Historical Development

The foundations of quadrature amplitude modulation (QAM) trace back to early 20th-century efforts to optimize signal transmission in telephony and radio. In 1915, John R. Carson, an engineer at AT&T, developed foundational mathematical descriptions of amplitude modulation and single-sideband techniques, enabling more efficient use of bandwidth by suppressing redundant carrier components and sidebands. These concepts influenced subsequent quadrature methods by demonstrating how multiple signals could be multiplexed on a single carrier using phase relationships. During the 1930s, radio transmission technologies advanced with explorations of combined and to enhance , particularly in long-distance and systems where bandwidth was limited. Engineers at and other firms experimented with orthogonal carriers to multiplex signals, setting the stage for QAM's dual-carrier structure. By the 1940s, amid , military drove innovations in robust modulation for and secure radio links, incorporating early forms of phase-shifted signals to improve reliability in noisy environments, though full QAM implementations remained nascent. The transition to digital QAM occurred in the 1960s, driven by the demand for higher-speed data transmission over telephone lines. At Bell Laboratories, Charles R. Cahn proposed the first practical digital QAM scheme in 1960, extending phase-shift keying by varying amplitudes on two quadrature carriers to encode multiple bits per symbol, achieving rates up to several kilobits per second. Bell Labs engineers, including Robert W. Lucky, further advanced this with adaptive equalization techniques in 1965, compensating for channel distortions to enable reliable QAM modems like early versions operating at 2400 bps. Contributions from AT&T pioneers such as Harold S. Black, whose 1927 invention of negative feedback amplifiers stabilized signal processing essential for QAM systems, supported these developments. Standardization efforts by the (ITU) formalized QAM in modem recommendations, such as V.29 in 1976, specifying 16-QAM for 9600 bps data rates. Early commercial digital QAM modems appeared in the early , exemplified by the 9600C introduced in 1971, which used QAM at 2400 for 9600 bps over leased lines. The IEEE later incorporated QAM into wireless standards, beginning with early definitions in the 1980s. A significant advancement came with the ITU V.32 standard in 1984, using trellis-coded 32-QAM for error-corrected data transmission at 9600 bps over dial-up lines, marking a shift toward mainstream .

Mathematical Description

Time-Domain Representation

The time-domain representation of a quadrature amplitude modulated (QAM) signal combines two signals onto orthogonal carriers to form the transmitted . The in-phase signal I(t)I(t) modulates a cosine carrier, while the quadrature signal Q(t)Q(t) modulates a sine carrier, resulting in the general form s(t)=I(t)cos(2πfct)Q(t)sin(2πfct),s(t) = I(t) \cos(2\pi f_c t) - Q(t) \sin(2\pi f_c t), where fcf_c denotes the carrier frequency. This expression arises from the need to transmit two independent information-bearing signals within the same frequency band without mutual interference. To derive this form, consider separate amplitude modulation of the carriers: the in-phase term I(t)cos(2πfct)I(t) \cos(2\pi f_c t) and the quadrature term Q(t)sin(2πfct)Q(t) \sin(2\pi f_c t). Adding these yields the QAM signal, with the negative sign on the sine term adopted for consistency with the complex exponential representation. The orthogonality of the carriers ensures no crosstalk, as the integral 0Tcos(2πfct)sin(2πfct)dt=0\int_0^{T} \cos(2\pi f_c t) \sin(2\pi f_c t) \, dt = 0 over one period T=1/fcT = 1/f_c, following the trigonometric identity sin(2θ)=2sinθcosθ\sin(2\theta) = 2 \sin \theta \cos \theta. This property allows the in-phase and quadrature components to be recovered independently at the receiver. An equivalent phasor representation employs the complex envelope g(t)=I(t)+jQ(t)g(t) = I(t) + j Q(t), such that the QAM signal is the real part of the modulated complex signal: s(t)=Re[g(t)ej2πfct].s(t) = \mathrm{Re} \left[ g(t) e^{j 2\pi f_c t} \right]. Expanding this confirms the earlier time-domain form, as Re[(I+jQ)(cos(2πfct)+jsin(2πfct))]=I(t)cos(2πfct)Q(t)sin(2πfct)\mathrm{Re}[(I + jQ)(\cos(2\pi f_c t) + j \sin(2\pi f_c t))] = I(t) \cos(2\pi f_c t) - Q(t) \sin(2\pi f_c t). This complex notation simplifies analysis of modulation processes. In analog applications, QAM modulates continuous-time baseband signals such as voice or video. For instance, in the NTSC color television standard, the chrominance signal is QAM-modulated onto a 3.58 MHz subcarrier, with the in-phase (I) and quadrature (Q) components carrying color information alongside the luminance signal. Due to carrier orthogonality, the effective bandwidth of the QAM signal equals that of a single baseband signal (approximately 2B2B Hz if each baseband has bandwidth BB), rather than doubling as in non-orthogonal schemes. This spectral efficiency enables two signals to share the channel without expansion.

Frequency-Domain Analysis

The frequency-domain representation of a quadrature amplitude modulation (QAM) signal is derived from its time-domain form, where the signal s(t)=I(t)cos(2πfct)Q(t)sin(2πfct)s(t) = I(t) \cos(2\pi f_c t) - Q(t) \sin(2\pi f_c t) undergoes Fourier transformation to yield S(f)=12[I(ffc)+I(f+fc)]+j12[Q(ffc)Q(f+fc)],S(f) = \frac{1}{2} \left[ I(f - f_c) + I(f + f_c) \right] + j \frac{1}{2} \left[ Q(f - f_c) - Q(f + f_c) \right], with I(f)I(f) and Q(f)Q(f) denoting the Fourier transforms of the in-phase and quadrature signals, respectively, and fcf_c the carrier frequency. This expression illustrates that the QAM comprises translated copies of the spectra centered symmetrically at ±fc\pm f_c, enabling efficient packing of information without requiring additional bandwidth beyond that of a single signal. Key spectral properties of QAM arise from this structure: in a balanced modulator, the absence of a DC component in I(t)I(t) and Q(t)Q(t) eliminates carrier leakage, preventing a discrete spectral line at fcf_c. The quadrature phase separation ensures minimal overlap between the upper and lower sidebands of the I and Q components, as the orthogonal carriers allow independent modulation while occupying the same frequency band. QAM achieves superior bandwidth efficiency by allowing two independent baseband signals, each of bandwidth BB, to be transmitted within a total bandwidth of 2B2B Hz, whereas transmitting them separately using conventional double-sideband (AM) would require 4B4B Hz. For random independent I and Q signals assuming uniform distribution, the power spectral density (PSD) of the QAM signal appears flat across the baseband width before upconversion, resulting in a passband PSD that mirrors this uniformity around fcf_c when the baseband signals are bandlimited. Filtering impacts the QAM significantly in analog implementations; an ideal rectangular filter produces a sinc-shaped with extending infinitely, potentially causing interference, whereas a introduces a controlled factor to confine energy within the desired band, minimizing emissions while preserving the core bandwidth efficiency.

Analog QAM

Modulation Process

The modulation process in analog quadrature amplitude modulation (QAM) begins with two independent baseband signals, denoted as the in-phase component I(t) and the quadrature component Q(t). These signals are processed through a transmitter structure that modulates them onto orthogonal carriers. Specifically, I(t) is multiplied by the cosine carrier wave, cos(2πf_c t), and Q(t) is multiplied by the negative sine carrier wave, -sin(2πf_c t), where f_c is the carrier frequency. The resulting signals are then summed to produce the composite QAM output s(t) = I(t) cos(2πf_c t) - Q(t) sin(2πf_c t). Key components of the transmitter include a that generates the carrier signal at f_c, which is subsequently split into two quadrature phases using a 90° hybrid splitter to provide the cos(2πf_c t) and sin(2πf_c t) references. Each signal drives a balanced modulator—typically implemented as a double-balanced mixer—that performs the while suppressing the carrier to eliminate unwanted carrier leakage in the output. The modulated I and Q components are combined using a 0° hybrid combiner before amplification and transmission. Practical implementation requires careful amplitude scaling of I(t) and Q(t) to balance power distribution between the channels for efficient transmitter operation and to maintain overall signal power within regulatory limits. Additionally, linear power amplifiers are essential following the combiner to preserve the amplitude and phase integrity of the modulated signal, avoiding nonlinear distortion that could introduce intermodulation products. A representative application of analog QAM is in FM radio broadcasting, where the left-plus-right audio signal (L + R) serves as the I(t) component modulating a 38 kHz subcarrier in-phase, and the left-minus-right signal (L - R) serves as the Q(t) component modulating the same subcarrier in quadrature; this composite is then frequency-modulated onto the RF carrier. Non-ideal conditions, such as gain imbalance between the I and Q paths or phase errors deviating from exact 90° quadrature, result in where components from one channel leak into the other, degrading channel separation and introducing interference.

Demodulation Techniques

Coherent demodulation is the primary technique employed to recover the in-phase (I) and quadrature (Q) components from a received analog QAM signal s(t)=I(t)cos(2πfct)Q(t)sin(2πfct)s(t) = I(t) \cos(2\pi f_c t) - Q(t) \sin(2\pi f_c t), where fcf_c is the carrier . This process requires with the carrier's phase and at the receiver. The received signal is first multiplied by 2cos(2πfct)2 \cos(2\pi f_c t) to extract the I component, yielding 2s(t)cos(2πfct)=I(t)+I(t)cos(4πfct)Q(t)sin(4πfct)2 s(t) \cos(2\pi f_c t) = I(t) + I(t) \cos(4\pi f_c t) - Q(t) \sin(4\pi f_c t), followed by low-pass filtering to isolate I(t)I(t). Similarly, multiplication by 2sin(2πfct)-2 \sin(2\pi f_c t) recovers the Q component as Q(t)Q(t) after low-pass filtering, removing the double- terms at 2fc2f_c. Carrier recovery is essential for coherent , as the receiver's must align in phase and frequency with the incoming carrier, which may suffer from offsets due to transmission impairments. A (PLL) achieves this synchronization by comparing the phase of the received signal (or a derived pilot tone) with the output, adjusting the latter through a feedback loop to minimize the phase error. For example, in FM stereo radio broadcasting, the 38 kHz subcarrier is recovered from the 19 kHz pilot tone by frequency doubling using a . Non-coherent methods, such as detection, are generally ineffective for QAM signals due to their reliance on phase information for distinguishing I and Q components; these techniques ignore phase variations, leading to irreducible errors in and phase recovery. The low-pass filters in coherent demodulation are designed with a equal to the baseband signal bandwidth BB, ensuring of the high-frequency components around 2fc2f_c while preserving the desired I and Q signals up to BB Hz. These filters, often implemented as analog Butterworth or Bessel types, balance sharpness and phase linearity to minimize in the recovered . Practical analog QAM demodulators must address imperfections like DC offsets, introduced by local oscillator leakage or mixer imbalances, which manifest as constant biases in the I and Q outputs and can be removed via high-pass filtering or adaptive subtraction using training sequences. Quadrature errors, arising from non-orthogonal local carrier signals (e.g., a phase mismatch ϕ90\phi \neq 90^\circ), cause crosstalk between I and Q channels; basic correction involves estimating the error through tones and applying a to align the axes, improving without digital processing.

Digital QAM

Constellation Diagrams

In digital quadrature amplitude modulation (QAM), the provides a visual representation of the possible transmitted as discrete points in the , where the horizontal axis denotes the in-phase (I) and the vertical axis denotes the quadrature (Q) . Each point corresponds to a unique pair of I and Q values, encapsulating both and phase information for the symbol. For an M-ary QAM scheme, the constellation comprises M points, typically arranged in a square lattice for standard implementations, with M\sqrt{M}
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