Singlet Halperin State Construction

In summary, the conversation discusses the construction of the singlet Halperin state in David Tong's Fractional Quantum Hall Effect notes. The confusion lies in the sentence "It can be seen to be a spin singlet because the last two factors are just Slater determinants for spin up and spin down respectively." The last two factors refer to ##\prod_{i<j \ \text{odd}}(z_{i}-z_{j})## and ##\prod_{k<l \ \text{even}}(z_{k}-z_{l})##, which are the slater determinants for spin up and spin down. However, there is confusion about whether these factors are antisymmetric, which could potentially cause a problem since the
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thatboi
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Hi all,
I'm reading through David Tong's Fractional Quantum Hall Effect notes right now and am stumped by how he constructs the singlet Halperin state (the last equation in this document: https://www.damtp.cam.ac.uk/user/tong/qhe/three.pdf, on page 116 as per the document page number at the bottom of each page). Specifically, I do not understand the sentence "It can be seen to be a spin singlet because the last two factors are just Slater determinants for spin up and spin down respectively, which is guaranteed to form a spin singlet." I assume that the "last two factors" are referring to ##\prod_{i<j \ \text{odd}}(z_{i}-z_{j})## and ##\prod_{k<l \ \text{even}}(z_{k}-z_{l})##. My 2 questions are:
i.) How do we see that these are the slater determinants of spin up and spin down? To me, they just look like the vandermonde determinant we see associated with the Laughlin states.
ii.) Aren't these factors antisymmetric? Wouldn't that the be a problem considering the spin states are already antisymmetric?
Thanks!
 

FAQ: Singlet Halperin State Construction

What is the Singlet Halperin State Construction?

The Singlet Halperin State Construction is a theoretical framework used in the study of quantum Hall effects, particularly in systems with multiple components, such as bilayer systems or systems with spin degrees of freedom. It describes a specific type of quantum Hall state that exhibits singlet pairing between particles in different components.

How does the Singlet Halperin State differ from other quantum Hall states?

The Singlet Halperin State is unique because it involves the formation of singlet pairs between particles in different components, leading to a specific type of correlated state. This is in contrast to single-component quantum Hall states, where the correlations are typically within a single component. The singlet pairing can lead to different topological properties and excitations.

What are the key mathematical tools used in the Singlet Halperin State Construction?

The construction of the Singlet Halperin State often involves the use of wavefunctions that incorporate symmetric and antisymmetric combinations of particle coordinates. Techniques from group theory, such as SU(2) symmetry, and methods from many-body physics, like the use of composite fermions or bosons, are also commonly employed to describe the state.

What physical systems can exhibit Singlet Halperin States?

Singlet Halperin States can be found in bilayer quantum Hall systems, where electrons are confined to two closely spaced layers, or in systems with spin degrees of freedom where electrons can form singlet pairs between different spin states. These states can also potentially occur in other multi-component systems where similar singlet pairings are energetically favorable.

What are the experimental signatures of the Singlet Halperin State?

Experimental signatures of the Singlet Halperin State include specific quantized Hall conductance values that differ from those of single-component states, as well as unique excitation spectra that can be probed through techniques like tunneling spectroscopy or transport measurements. Additionally, the presence of interlayer coherence in bilayer systems can be a strong indicator of such states.

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