# How do ZOR antennas work?

In a Dialog application note (AN-B-027), I ran into this rather curious antenna for 2.4GHz operation:

This is on two PCB layers connected with vias; the whole thing is shorted together at DC, but forms a sort of labyrinth pattern that switches back and forth between the layers.

How does it work? The overall operating principle is a bit beyond me. Is it basically a monopole with a bunch of inductors (the vias) used to load it? Something else?

Why would one want to use this type of PCB trace antenna as opposed to something more common like PIFA or MIFA? What are the pros and cons?

• it looks more like two single turn coils wound in opposite directions placed side by side Nov 9, 2019 at 1:21
• @jsotola Yes, but they're also shorted together at both ends. I think if this was a loop (or double loop) antenna, it would have to be fed differently... Nov 9, 2019 at 1:38
• Wow. ZOR = Metamaterial.
– JRE
Dec 2, 2019 at 20:04
• How is it simplest case different from a 2OR? second order\ Dec 6, 2019 at 12:42
• @TonyStewartSunnyskyguyEE75 I'd like a definite answer to that myself. From various sources I've found, it seems that ZOR means the resonant frequency of the structure does not depend on its size, but I don't really understand the physical basis behind that. Most normal antennas would be first order (quarter-wave), or second order (3/4 wave). Dec 8, 2019 at 7:45

I have to disagree with this answer to this question.

That answer has conflated electrically short antennas with ZOR antennas, and then primarily discusses electrically short antennas rather than ZOR antennas.

First, this really needs to be addressed:

"ZOR" is a complicated way of saying "electrically small" or "electrically short" resonant antenna (or antenna-array.)

This is absolutely incorrect. ZOR antennas have nothing to do with electrically short antennas, these two terms are not interchangeable, and they mean completely different things.

I want to be clear that the name 'ZOR antenna' is in itself a near misnomer. Specifically, the antenna part. They are antennas in function only. They receive and radiate electromagnetic waves, but that is where the similarities to more familiar antennas end. They are nothing like resonant or non-resonant antennas and work via an exotic mechanism that is absent entirely in resonant antennas or electrically short antennas like an AM radio antenna.

the antennas inside old AM transistor radios are simple 1-element ZOR antennas

And an AM radio antenna is in absolutely no way a ZOR antenna. In fact, there is no such thing as a 'single-element' ZOR antenna. Having multiple elements is fundamental to the very operation and definition of a ZOR antenna, so there is no such thing as one with 1-element. But even taking that aside, an AM radio antenna is not even a single element of a ZOR antenna. It is just an electrically short antenna, that is all.

Instead it works by reaching out into surrounding space, and focusing rf waves onto itself!

Sorry, but this is nothing but hand-waving. No antenna, ZOR or otherwise, works by 'focusing rf waves onto itself' any more than a lens could be made to focus light onto itself. If that were possible, you wouldn't even need a lens in the first place.

The proposed mechanism of how even regular antennas work isn't correct either:

all antennas work by producing an EM field, and the actual receiving process is done by the interacting fields.

This description of how antennas work is egregiously incorrect, but does give a good lead-in to do a deep dive on how antennas work, which is really a preqrequisite to discuss ZOR antennas. We'll get there, just bear with me.

No antenna works by producing an electromagnetic field. Nor is the receiving process done by electromagnetic fields interacting. This should be immediately obvious as electromagnetic fields do not interact with each other, they simply become additively superimposed on each other. This is apparent in every aspect of circuit design as well as daily life. If you turn on two light bulbs in a room, it gets brighter but the illumination pattern of each light bulb individually does not change, they are simply added to the extent they overlap. If you use a DC voltage to bias (or put another way, superimpose on top of) an AC waveform, you simply shift that waveform that many volts relative to the DC's ground. It does not actually alter the AC waveform in anyway. This is widely used for things like phantom power in professional audio, or as a basic building block of signal conditioning.

If electromagnetic fields interacted with other electromagnetic fields, none of those things would work or behave like they behave all the time in day-to-day life. But don't take my word for it, take Maxwell's.

Maxwell's equations are a system of linear equations, and any linear equation or system of related linear equations can be shown by mathematical proof to adhere to the superposition principal. All electromagnetic wave solutions are simply added together, the presence of one or any other number of additional EM waves has no effect on any others. EM waves behave completely independently of each other. Essentially, there is a mathematical proof that makes the described mechanism behind antennas impossible.

Everything that antennas do are thanks entirely to mobile charge carriers within them. Ultimately, you just need electrons that are able to move and aren't bound to an atomic nucleus as valance charge. Conductors provide a convenient form of movable electrons in the form of a conductive material's conduction band.

Electromagnetic waves are made whenever an electron is accelerated. Not in motion, but actively having that motion changed, better known as acceleration. This is important. A moving electron radiates no electromagnetic waves, but one whose rate of movement is changing (is being accelerated) will radiate electromagnetic waves. What they are really radiating away is momentum from this acceleration. So this is reciprocated when an electron absorbs an electromagnetic wave. This also results in momentum transfer, causing said electron to be accelerated by that wave. There is no difference between transmitting and receiving in antennas, one is simply the time-reversal symmetry of the other. If you watched a transmitting antenna but with time flowing the opposite direction, it would not be distinguishable from that same antenna receiving the same wave. Transmitting and receiving is the same process, only the sign of the progress in time is opposite.

There seems to be a serious misconception that antennas must be similar in size to their intended wavelength, and if they are not, then that cannot really interact with much larger electromagnetic waves.

These are waves. Having a wavelength the size of a mountain doesn't mean the wave is some mountain-sized object and you need a similarly sized thing to even interact with it. This is not the case at all. An electromagnetic wave, as it passes by, will oscillate between an electric field and a magnetic field moving through free space. What happens to electrons in the presence of an electric field? They get accelerated. Longer wavelengths will induce smaller and smaller voltages across a conductor of fixed size due to the potential being stretched out over a longer wavelength, but this just reduces the induced voltage in the antenna.

This does of course translate into the dependence seen in conventional antennas, of course. But this dependence is not nearly as severe as it is made out to be. What antenna size ultimately influences is something called radiation resistance. Or in the context of transmission instead of reception, source resistance. It is the same thing in either case.

It is measured in ohms, and it opposes and dissipates energy in an antenna when the charge carriers (electrons) are being accelerated by an electric field within that antenna - be it a voltage produced by a transmitter, or a voltage produced by an electromagnetic wave received by the antenna. When this occurs, just like with any acceleration of an electron, this causes the electron to radiate away some of that momentum in the form of an electromagnetic wave. This causes a recoil force in the momentum of the electron, which both acts to resist the direction of current as well as dissipate energy, so it behaves just like real resistance, with the exception that the energy is dissipated as electromagnetic waves instead of heat due to resistance in the antenna itself.

This also means that an electron that is accelerated by an electromagnetic wave will radiate one as well. An ideal superconducting antenna will, as a result, only ever absorb and convert into electrical current half of the received power of electromagnetic waves. The other half is reradiated back to the source. This is the same thing that happens with reflection in a transmission line due to impedance change. You can view this as an impedance mismatch if you wish. All of what I am describing have several different equally valid 'viewpoints' from which you can view it from, but they all describe the same process, just by focusing on different aspects. Momentum, impedance, refraction (I'll be getting to that!), pick your poison, it's all the same thing seen from different angles.

The important thing to understand here is that as the radiation resistance can be thought of as energy lost via the radiation of electromagnetic waves. Too much (an antenna which is longer than the resonant frequency length) makes it harder to push the electrons, while too low (electrically short) and there stops being enough resistance to dissipate much power - and thus the radiated power of electromagnetic waves is reduced for a given current. The left over power is reflected back to the transmitting antenna/source, rather than usable by any sort of radio receiver.

Radiation/source resistance, for a simple monopole or dipole antenna, below the optimal resonant length ( $$\ \frac{λ}{2} \$$ for a monopole, or $$\ \frac{λ}{4} \$$ for a dipole), decreases with the square the length shorter than this resonant length. This is an electrically short antenna. You can still make it resonant with the desired frequency by 'electrically lengthening' the antenna using reactive components to influence the resonant frequency. This is what is done with an AM antenna. There is no magic here - AM antennas are, to put it bluntly, terrible. But back in AM radio's heyday, the frequencies were also so low that amplifiers capable of amplifying the tiny amount of signal such a garbage antenna could even receive to useful levels became practical to build with the available technology. There is no zero-order resonance or any other hand-waving magic going on with AM radio antennas. They're terrible antennas by every possible measure. But it was more important that the frequencies be low back then, and the combination of antenna and amplifier was the combination that worked.

OK, finally, we can get to

## ZOR Antennas

So what are they? What does 'zero-order resonance' even mean?

You should be sitting down, because the answer is, frankly, mind-blowing.

At the simplest, ZOR Antennas are simply transmission lines - but not ordinary ones. A ZOR antenna is really just another name for what are known as Composite Right-Left Handed (CRLH) transmission lines. Superficially, they are transmission lines that are periodically loaded with series capacitors and parallel/shunt inductors. These periodic structures, individually, are referred to as 'unit cells'. A ZOR antenna requires, at a minimum, 2 of these unit cells to function. There are no single element ZOR antennas.

Let's back up for a minute. Let's stop even talking about radio. Let's talk about light. Specifically, refraction of light.

When a wave changes mediums and there is a difference in the propagation speed between those mediums, the direction of that wave is bent as a result. This is called refraction. The principle upon which lenses, prisms, mirages, etc all depend on:

Light is an electromagnetic wave, and refraction also relates to the permittivity (how strongly a material's electric dipoles will polarize in the presence of an electric field) and permeability (how strong a material will magnetize in to a magnetic field) of a material. This relation is fairly simple. The refractive index of a material, $$\ n \$$, (which is how much the wave's propagation is bent), can be calculated entirely from permittivity ($$\ \epsilon \$$) and permeability ($$\ \mu \$$) thus: $$\ n = \sqrt{ \epsilon \mu } \$$.

Imagine for a moment if we could make a material that had negative permeability. What would this even mean? A material with negative permeability would produce a magnetic response to an electric field. And likewise for negative permittivity, this would mean that a magnetic field would induce an electric field in a material. Such behavior is quite bizarre and not found in nature. But it is found in something we electrical engineers use all the time.

LC tanks. An LC tank causes an electric field in a capacitor to move charge, producing current, which induces a magnetic field through a parallel or series connected inductor. And a magnetic field will cause an electric field to appear across the plats of a capacitor due to the induced current moving charge onto and off of those plates.

It really is that easy. One can effectively realize negative permittivity and permeability in this way simply by using micro strips to produce parasitic lumped components in periodic structures.

But why?

When both of these are negative, something amazing happens.

The refractive index becomes negative. Again, there are many ways you can view what this means, and they're all valid. This means that waves will be reflected antiparallel (backwards), but with a reversed phase. This means that the wave propagating backwards looks the same as that wave propagating forwards. This means the phase velocity is infinite. It looks like the wave isn't propagating at all.

Remember those waves that get reradiated/reflected back to the source due to radiation resistance? If you have a negative refraction index, those waves can radiated in the opposite direction. The radiation is in the direction back into the receiving antenna that is doing the reradiating. Put another way, that energy is no longer lost to redadiation, but is instead stored, as inductors and capacitors tend to do. This has the amazing effect of allowing all of the electromagnetic energy to be captured by the antenna, regardless of the size and without any dependence on resonance.

Zeroth-order resonance isn't resonance at all, but instead is referring to the propagation constant in these antennas being zero due to this reversal. The wave stops, its phase velocity is infinite, it doesn't propagate, it is simply captured. The momentum of the electrons is still in the opposite direction than the momentum it is counteracting - momentum is still conserved - but by the time that reradiation of momentum in the form of an electromagnetic wave occurs, the wave was been reflected and now that momentum aids the current instead of fighting it.

Zeroth-order antennas are also known as metamaterial antennas. They don't just allow the construction of small antennas, they allow construction of arbitrarily small antennas with far wider bandwidths than is possible with conventional antennas.

Simply put, ZOR antennas can do what is impossible with conventional antennas. Using these periodic structures, we are no longer bound by wavelength. ZOR antennas remove the space dependence of electromagnetic reception, leaving only time.

In the optical domain, they could be used to resolve images beyond the diffraction limit. In the electromagnetic domain, they can be said to focus waves onto themselves, but really, they are reflecting the waves back into themselves.

"ZOR" is a complicated way of saying "electrically small" or "electrically short" resonant antenna (or antenna-array.) It's like having a CB-radio resonant base-load, but without any whip-antenna. Or, it's like using a giant single hydrogen atom as your antenna. It's a fascinating topic, a weird little niche in antenna-theory, and not necessarily math-heavy.

For example, the antennas inside old AM transistor radios are simple 1-element ZOR antennas (and the tuning knob of those receivers had a variable capacitor hooked right across the ferrite-core antenna-coil.) The AM antenna is actually a passive LC tank-circuit. Unlike with broadband 1/4-wave whip antennas (FM band,) the AM ferrite loopstick is far smaller than 1/4-wave, and sharply resonates with the station being received.

Radio hams are familiar with this effect: their 160M mobile rigs don't need any 80-meter tower sticking out of the car, instead they have a short whip antenna with a high-Q LC resonator using a motorized tuning cap, and the EA Effective Aperture is enormous, far larger than the physical antenna size. It works great as a receiver (or in other words, the trick is not just to use a transmitter to overdrive a too-small antenna. It's far weirder than that.)

Another more modern example is the phone antenna, mini "chip antenna" or "ceramic antenna" 5mm wide, far smaller than patch antennas, and employing a tiny high-Q resonator. See a recent discussion: How does a chip antenna work?. The higher the Q of the sub-wavelength sized resonator, the larger is the "EA" Effective Area, or Effective Aperture (or "virtual size.") In theory, down at VLF, a 10cm antenna could behave the same as as a KMs-long antenna, if only the resonator resistance could be low enough, for immense Q-factor (use superconductor?)

The real "magic" happens when we employ a high-Q resonator coil where its diameter is NOT a half-wavelength, but instead far smaller. Yet still it behaves as if its physical extent was half-wavelength. Whenever tuned to the received frequency, the tiny antenna intercepts some major microwatts, as if it could magically reach far out into space, and focus the rf waves onto itself. With AM radios, the coil might be a couple cm long, yet 500KHz radio waves have HUNDRED-FIFTY METER wavelenth! How can such a tiny device hope to absorb any rf energy? Doesn't it need a receiver front-end with immense gain and impossible SNR? Instead it works by reaching out into surrounding space, and focusing rf waves onto itself! No joke. Sharply resonant circuits behave as "EM wave-funnels." They have an EA, Effective Aperture, which is anomously enormous. One physics paper dubbed this the "Energy-sucking Antenna" effect.

Apparently the details in this part of antenna-theory were missed during the early decades, and only discovered in the mid-1980s. Authors calculated the pattern of rf propagation around small antennas, as below. Some of the Poynting-vector flux passes by, but the flux coming too close gets diverted and "sucked in." Conclusion: a tiny point-like antenna can behave just like a half-wave dipole antenna, if the tiny antenna is a tuneable resonator with extremely high Q-factor.

The TDLR: all antennas work by producing an EM field, and the actual receiving process is done by the interacting fields. So, reduce the size of your loop antenna while cranking up the current, so the b-field doesn't decrease. Or, reduce the size of your whip antenna while raising the drive voltage, so the e-field doesn't decrease. A high-Q resonator accomplishes this automatically. Metal resistance and Q-factor are of course a major limitation, otherwise we could broadcast megawatts using resonant antennas the size of molecules.

With the PCB antenna-traces in your example above, every via and trace is inductive. There must be some significant capacitance too, in order to change the "coil" traces into a sharp-tuned resonator. That's probably the reason they've placed traces laying against each other across the facing sides of the PCB. The PCB thickness and dielectric constant would need tight control, to place the antenna's resonance on the desired WiFi peak. (Or, I guess they could just add a Pi-match stage, and chose the cap values to adjust the driver impedance to the actual antenna, even if it's not broadcasting right at the resonant peak.)

Your antenna might be a simple LC tank circuit. In that case its second floating terminal is positioned away from the groundplane, and two parallel coils used to give higher Q-factor, like using Litz-wire to wind a single coil. The spectrum would be a single deep notch. Or, sometimes designers perform some fancy tricks with multiple resonant frequencies (to use one single antenna at very different bands.) Or perhaps it has multiple resonators at the same frequency, to create some 3D antenna-lobes with very different shape than a simple dipole.

Or, maybe they let an AI (neural network sw) perform an evolution-algorithm on a piece of bent wire, finally producing that weird shape. In that case it behaves as the end-goal requires, but nobody has a good idea on how it actually works!

:)

I've seen the ZOR version of beam-antennas, which behave much like Yagi-Uda antennas or log-periodic (or like ceramic-cone waveguide elements.) But rather than using halfwave dipole elements, they use extremely tiny resonators, positioned in a row. Search term: waveguide antenna.

http://amasci.com/tesla/dipole1.html

Old products based on this weird effect are still around: the passive "amplifiers" for AM radio receivers. Look up "Select-A-Tenna," or the Terk AM booster. These were simple RLC resonant tank circuits, with a heavy many-turn loop antenna for high Q, and a variable capacitor for tuning. Just place it near your AM radio, tweak it and aim it for maximum reception.

That recent crazy MIT stuff with "evanescent-wave" wireless broadcast power ...it's using the same physics as above. They give it a fancy name, but really it's just a pair of sharp-tuned resonators, with the coil-size far smaller than quarter-wavelength. (And of course, rf transformers with tuned-primary, tuned-secondary, they harness the same effect. That's why you'll see such transformers in high-KW transmitters, producing unexpectedly high coupling between coils, but without needing any ferrite core.)

All the weird ZOR stuff you'll see in various research papers ...they get crazy, because each element is essentially a giant atom, as if they're building molecular arrays made from PCB traces. It's not "antennas" anymore; it's few-Torr Sodium vapor appearing totally opaque black in yellow Sodium light, it's spectrographic emission lines and absorption bands in crystals. (Heh, if made from superconductor and dunked in liquid helium, they'd be true QM objects, with photon statistics and everything.)

• A "point-like resonant absorber" sounds like a leap of faith in Maxwellian or even molecular analysis. Like flux capacitor in series resonance with dangling inductive participle sucking up aether, WHy is this not a 2nd order filter with a Q >100 " reaching out into surrounding space, and focusing rf waves onto itself!" sound slike science fiction Dec 9, 2019 at 0:59
• @TonyStewartSunnyskyguyEE75 and... that's why this topic was little-explored until the 1980s! It seems like science fiction. (n.b. "point like" just means the antenna size << wavelength, as when atoms absorb 500nM light, or when a foot-wide AM loop-antenna can intercept enough milliwatts to run a crystal earphone.) Dec 9, 2019 at 1:27
• @TonyStewartSunnyskyguyEE75 Search topic "electrically-short resonant antennas." The idea is found throughout physics. Even crystal radios employ this effect (the resonator ISN'T a filter as usually stated, since without the resonator, all stations should be heard, yet in fact, no signal is heard.) Similar idea: a wire antenna shouldn't be able to receive, since the wire is far too thin to block any meters-wide EM waves. But even #40 wire is an excellent antenna for longwave. By that reasoning, if "one-dimensional" wire intercepts major RF energy, so can a 0-dimensional antenna. Works fine! Dec 9, 2019 at 1:42
• This sounds like some fascinating Deep Magic. Dec 10, 2019 at 2:53
• @Hearth antenna design was always a Black Art. This small-resonator stuff is even blackerer! We can use it to explain the Director elements in Yagi, and anomalous resonant noncontact friction, and Stimulated Emission wo/QM concepts, and also the NSOM scanning microscope (the word "nearfield" is a dead giveaway.) Also, needless to say, it's how Nikola Tesla planned to receive the watts of Broadcast Power at 10KHz without every receiver needing a quarter-wave vertical (He's operating down in the... "fifteen-kilometer band!" Dunk yr tank-circuit in a tank of Tesla's Liquid Air.) Dec 11, 2019 at 3:50