Introduction
In our previous lessons, we have constructed a description of the electron's state in an atom using three quantum numbers:
- , the principal quantum number, defining the energy level and size.
- , the azimuthal quantum number, defining the orbital's shape.
- , the magnetic quantum number, defining the orbital's spatial orientation.
These three numbers emerge from solving the Schrödinger equation and seem to paint a complete picture of the electron's probability wave, its "orbital." However, a series of puzzling experimental results in the early 20th century revealed that this picture was incomplete. There was another property of the electron, one that had nothing to do with its motion in space, that was crucial to its identity.
Today, our goal is to uncover this fourth and final quantum number, electron spin (). We will explore the experimental evidence that demanded its existence and come to understand it not as a simple rotation, but as an intrinsic, non-classical property that is fundamental to the very structure of matter.
1. The Breakdown of the Classical Analogy
When experiments first suggested that electrons possess their own intrinsic magnetic moment, the most intuitive explanation was to imagine the electron as a tiny, spinning sphere of charge. Classical electromagnetism tells us that a rotating charge creates a magnetic field, so this "spin" seemed like a reasonable physical model.
However, this simple mental model catastrophically fails when inspected with the rigor of physics. Let's explore why.
First, let's consider the idea of "spin" from a first-principles perspective. What does it mean for something to spin?
I never understood why electrons have spin... until now!
The channel FloatHeadPhysics offers a sharp, logical argument for why a truly fundamental particle, like an electron, cannot 'spin' in the classical sense. This will help us dismantle the intuitive but incorrect analogy from the ground up.
Please watch the first 4 minutes and 20 seconds of this video. Focus on the core argument: spin is defined as the coordinated circular motion of a group of particles around a common center. A fundamental particle, by definition, is not a group of particles, and therefore the concept of classical spin cannot apply to it.
This logical argument is compelling on its own. But the problem becomes even more severe when we consider the quantitative implications. Physicists like Wolfgang Pauli calculated that for a particle with the electron's charge and point-like size, the surface would have to rotate faster than the speed of light to produce the experimentally observed magnetic moment. This would violate the theory of special relativity.
The following video discusses the experimental context (the anomalous Zeeman effect) that hinted at a missing property and elaborates on Pauli's refutation of the classical spin model.
The PBS Space Time video 'Electrons DO NOT Spin' provides historical context and explains the fatal flaw in the classical spinning-sphere model.
Watch from 02:25 to 04:47. Pay close attention to two things: The mention of the 'anomalous Zeeman effect' as an experimental puzzle that the existing theory couldn't explain. The explanation of Wolfgang Pauli's argument that a classically spinning electron would require superluminal (faster-than-light) speeds.
So we are at an impasse. The classical model of a spinning electron is logically and physically untenable. And yet, experiments insist that electrons possess an intrinsic angular momentum and an associated magnetic moment. This forces us to abandon the classical analogy and seek a purely quantum mechanical explanation.
2. The Stern-Gerlach Experiment: Direct Evidence of Quantized Spin
The most direct and conceptually clean demonstration of this new property came from the Stern-Gerlach experiment, performed in 1922.
The setup is as follows:
- A beam of silver atoms is generated in an oven.
- This beam is passed through a non-uniform magnetic field.
- The deflection of the atoms is recorded on a detector screen.
A silver atom has 47 electrons. The first 46 form a stable, closed shell with zero net angular momentum. The 47th electron is in a 5s orbital (), meaning it has no orbital angular momentum. Therefore, any magnetic moment the atom possesses must come solely from the intrinsic properties of this single, outer electron.
Classical Prediction: If the electron's intrinsic magnetic moment could point in any random direction (as a classical magnet can), the atoms would be deflected by varying amounts, creating a continuous smear on the detector.
Experimental Result: The beam split into exactly two distinct spots.

This result is profound. It demonstrates that the electron's intrinsic magnetic moment is quantized. It can only align itself in two possible ways relative to the external field.
The next video segment explains this crucial experiment and its interpretation.
Let's return to the PBS Space Time video to see a clear animation and explanation of the Stern-Gerlach experiment.
Watch from 05:08 to 07:37. Focus on the contrast between the expected classical result (a continuous blur) and the observed quantum result (two discrete spots). This is the core experimental justification for spin.
3. The Spin Quantum Number ()
To account for this two-valuedness, a fourth quantum number was introduced: the spin magnetic quantum number, .
- It can take only two possible values: and .
- These are often referred to as "spin-up" and "spin-down," corresponding to the two beams in the Stern-Gerlach experiment.
This property is called spin, but we must constantly remind ourselves that this is just a name. It is an intrinsic angular momentum—a fundamental, unchangeable property of the electron, like its mass or charge, not a description of its motion. For any electron, its total intrinsic spin is characterized by a spin quantum number . The measurable component along an axis, , can then be or .
Particles with half-integer spin () are called fermions. Electrons, protons, and neutrons are all fermions. Particles with integer spin () are called bosons. Photons are bosons. This distinction, as we will soon see, is one of the most important in all of physics.
4. The Deeply Non-Classical Nature of Spin
The quantization into two states is strange enough, but the true nature of spin is even more alien to our classical intuition. The mathematical objects used to describe spin, called spinors, have bizarre rotational properties.
While a classical object (or a vector, or an integer-spin boson) returns to its original state after a 360° rotation, a spin- fermion does not. Its wavefunction acquires a negative sign. It requires a full 720° rotation to return to its original state.
This has no classical analogue. It's as if the electron is connected to the rest of the universe in a way our macroscopic senses cannot perceive.
To get a feel for this deeply strange property, let's watch the final segment from PBS Space Time, which introduces spinors and the famous 720-degree rotation analogy.
Watch from 07:37 to 10:22. Don't worry about understanding the full mathematics of spinors. Focus on the conceptual takeaway: the 'Feynman mug trick' or the 'plate trick' are physical analogies for how an object can be 'aware' of its orientation in a way that requires two full rotations to reset. This is a glimpse into the abstract world that spin inhabits.
This "weirdness" is not just a mathematical curiosity. As noted in a discussion on Physics Stack Exchange, this property is directly linked to one of the most fundamental principles of nature.
Does spin really have no classical analogue? - Physics Stack Exchange
A highly-rated answer on Physics Stack Exchange connects this abstract idea of spinors to a concrete physical law. This provides a crucial insight into why spin is so important.
Please read the response by the user 'Quillo'. Focus on the final paragraph under the heading '"Spin is quantum mechanical": in which sense?'. The key takeaway is the connection made between spin and the spin-statistics theorem. This theorem states that particles with half-integer spin (like electrons) must obey the Pauli Exclusion Principle. This is the 'necessity' for spinors in quantum mechanics.
This connection is the perfect bridge to our next topic. The strange, non-classical, two-valued nature of spin is not a minor detail. It is the deep reason why electrons in an atom arrange themselves the way they do.
Conclusion
Today we have added the fourth and final quantum number, , to our description of the electron. We now have a complete "quantum address" for an electron in an atom, specified by the four-part set: ().
Key Takeaways:
- The classical model of a spinning electron is physically impossible, as it would require faster-than-light rotation.
- The Stern-Gerlach experiment provided direct, irrefutable evidence that an electron's intrinsic magnetic moment is quantized, having only two possible orientations ("spin-up" and "spin-down").
- We describe this property with the spin magnetic quantum number, , which can be or .
- Spin is an intrinsic property, like mass or charge, not a form of mechanical motion. It is described by mathematical objects called spinors, which require a 720° rotation to return to their original state, highlighting its deeply non-classical nature.
We've established that the Schrödinger equation gave us the first three quantum numbers, which define the orbital (the electron's "house"), while spin is an intrinsic property of the electron itself (the "resident").
In our next lesson, we will introduce the Pauli Exclusion Principle. This principle uses the full set of four quantum numbers to state the fundamental rule of atomic architecture: no two electrons in an atom can have the same quantum address. This simple rule, born from the strange nature of spin, is the key to building the entire periodic table of elements.