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The most common general symptom of having the spins is described by its name: Diplopia double vision or polyplopia are common, as well as the symptoms of motion sickness and vertigo.
Ingesting a great deal of alcohol in a short amount of time causes alcohol to quickly enter the bloodstream. Mixing alcohol with normal soft drinks , rather than diet drinks delays the dizzying effects of alcohol because the sugary mixture slows the emptying of the stomach, so that drunkenness occurs less rapidly.
The dizzying effects of alcohol  upset the fragile mechanism that the inner ear uses to balance. Balance in the body is monitored principally by two systems, both of which are affected by alcohol sending abnormal impulses to the brain, [which tells it] that the body is rotating, causing disorientation and making the eyes spin round to compensate.
This "upset" has been seen in experiments in which human subjects were given clinical tests of the vestibular system before and after ingesting alcohol.
The spins are often reported when alcohol is mixed with cannabis , since both may cause dizziness  and magnify each other's effects.
Since at least some of the symptoms of "the spins" can be attributed to alcohol's disturbance of the vestibular system, many symptom relief strategies are based on increasing the body's ability to use other senses to regain balance.
In addition to the vestibular system, vision and touch information from the body are extremely important in maintaining balance.
In fact, the vestibular system is not necessary at all to maintain standing balance unless information from the other two systems becomes inadequate.
Keeping one foot flat on the ground while trying to sleep is one popular self-treatment for people whose dizziness is exacerbated by lying down with eyes closed.
One way to mask the symptoms of the spins is to avoid staring at moving objects, such as people who are dancing or ceiling fans. Instead, it helps to stare at a non-moving object and slowly blink a few times.
However, it will make things worse to keep one's eyes closed for an extended period. In minor cases of the spins, simply sitting alone in a quiet place or taking a walk is all it takes to make them subside.
When combined with the spin-statistics theorem , the spin of electrons results in the Pauli exclusion principle , which in turn underlies the periodic table of chemical elements.
Wolfgang Pauli in was the first to propose a doubling of electron states due to a two-valued non-classical "hidden rotation". When Paul Dirac derived his relativistic quantum mechanics in , electron spin was an essential part of it.
As the name suggests, spin was originally conceived as the rotation of a particle around some axis. This picture is correct so far as spin obeys the same mathematical laws as quantized angular momenta do.
On the other hand, spin has some peculiar properties that distinguish it from orbital angular momenta:. The value of s for an elementary particle depends only on the type of particle, and cannot be altered in any known way in contrast to the spin direction described below.
The spin angular momentum, S , of any physical system is quantized. The allowed values of S are. In contrast, orbital angular momentum can only take on integer values of s ; i.
The two families of particles obey different rules and broadly have different roles in the world around us. A key distinction between the two families is that fermions obey the Pauli exclusion principle ; that is, there cannot be two identical fermions simultaneously having the same quantum numbers meaning, roughly, having the same position, velocity and spin direction.
In contrast, bosons obey the rules of Bose—Einstein statistics and have no such restriction, so they may "bunch together" even if in identical states.
Also, composite particles can have spins different from their component particles. For example, a helium atom in the ground state has spin 0 and behaves like a boson, even though the quarks and electrons which make it up are all fermions.
The spin-statistics theorem states 1 that particles with half-integer spin fermions obey Fermi—Dirac statistics and the Pauli Exclusion Principle, and 2 that particles with integer spin bosons obey Bose—Einstein statistics, occupy "symmetric states", and thus can share quantum states.
The theorem relies on both quantum mechanics and the theory of special relativity , and this connection between spin and statistics has been called "one of the most important applications of the special relativity theory".
Particles with spin can possess a magnetic dipole moment , just like a rotating electrically charged body in classical electrodynamics.
These magnetic moments can be experimentally observed in several ways, e. For exclusively orbital rotations it would be 1 assuming that the mass and the charge occupy spheres of equal radius.
The electron, being a charged elementary particle, possesses a nonzero magnetic moment. In particular, the neutron possesses a non-zero magnetic moment despite being electrically neutral.
This fact was an early indication that the neutron is not an elementary particle. In fact, it is made up of quarks , which are electrically charged particles.
The magnetic moment of the neutron comes from the spins of the individual quarks and their orbital motions. Neutrinos are both elementary and electrically neutral.
The minimally extended Standard Model that takes into account non-zero neutrino masses predicts neutrino magnetic moments of: New physics above the electroweak scale could, however, lead to significantly higher neutrino magnetic moments.
The measurement of neutrino magnetic moments is an active area of research. In ordinary materials, the magnetic dipole moments of individual atoms produce magnetic fields that cancel one another, because each dipole points in a random direction, with the overall average being very near zero.
Ferromagnetic materials below their Curie temperature , however, exhibit magnetic domains in which the atomic dipole moments are locally aligned, producing a macroscopic, non-zero magnetic field from the domain.
These are the ordinary "magnets" with which we are all familiar. In paramagnetic materials, the magnetic dipole moments of individual atoms spontaneously align with an externally applied magnetic field.
In diamagnetic materials, on the other hand, the magnetic dipole moments of individual atoms spontaneously align oppositely to any externally applied magnetic field, even if it requires energy to do so.
The study of the behavior of such " spin models " is a thriving area of research in condensed matter physics. For instance, the Ising model describes spins dipoles that have only two possible states, up and down, whereas in the Heisenberg model the spin vector is allowed to point in any direction.
These models have many interesting properties, which have led to interesting results in the theory of phase transitions.
In classical mechanics, the angular momentum of a particle possesses not only a magnitude how fast the body is rotating , but also a direction either up or down on the axis of rotation of the particle.
Quantum mechanical spin also contains information about direction, but in a more subtle form. Quantum mechanics states that the component of angular momentum measured along any direction can only take on the values .
Conventionally the direction chosen is the z -axis:. This vector then would describe the "direction" in which the spin is pointing, corresponding to the classical concept of the axis of rotation.
It turns out that the spin vector is not very useful in actual quantum mechanical calculations, because it cannot be measured directly: However, for statistically large collections of particles that have been placed in the same pure quantum state, such as through the use of a Stern—Gerlach apparatus , the spin vector does have a well-defined experimental meaning: As a qualitative concept, the spin vector is often handy because it is easy to picture classically.
For instance, quantum mechanical spin can exhibit phenomena analogous to classical gyroscopic effects. For example, one can exert a kind of " torque " on an electron by putting it in a magnetic field the field acts upon the electron's intrinsic magnetic dipole moment —see the following section.
The result is that the spin vector undergoes precession , just like a classical gyroscope. This phenomenon is known as electron spin resonance ESR.
The equivalent behaviour of protons in atomic nuclei is used in nuclear magnetic resonance NMR spectroscopy and imaging. Mathematically, quantum-mechanical spin states are described by vector-like objects known as spinors.
There are subtle differences between the behavior of spinors and vectors under coordinate rotations. To return the particle to its exact original state, one needs a degree rotation.
The Plate trick and Möbius strip give non-quantum analogies. A spin-zero particle can only have a single quantum state, even after torque is applied.
Rotating a spin-2 particle degrees can bring it back to the same quantum state and a spin-4 particle should be rotated 90 degrees to bring it back to the same quantum state.
The spin-2 particle can be analogous to a straight stick that looks the same even after it is rotated degrees and a spin 0 particle can be imagined as sphere, which looks the same after whatever angle it is turned through.
Spin obeys commutation relations analogous to those of the orbital angular momentum:. It follows as with angular momentum that the eigenvectors of S 2 and S z expressed as kets in the total S basis are:.
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