Chosen Fixed Point
Here is the data for the chosen fixed point.
$F_{UV}$ represents the flavor symmetries in the UV Lagrangian, and $F_{IR}$ represents the flavor symmetries in the IR. $F_{UV}$ and $F_{IR}$ can differ due to accidental symmetry enhancement.
The number of marginal operators, $n_{marginal}$, minus the dimension of flavor symmetries in IR, $|F_{IR}|$, corresponds to the coefficient of $t^6$ in the superconformal index.
# | Theory | Superpotential | Central charge $a$ | Central charge $c$ | Ratio $a/c$ | Matter field: $R$-charge | U(1) part of $F_{UV}$ | Rank of $F_{UV}$ | Rational |
---|---|---|---|---|---|---|---|---|---|
47116 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{2}M_{4}$ + ${ }q_{2}^{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{3}M_{5}$ | 0.5221 | 0.6072 | 0.8599 | [X:[1.3333], M:[0.9724, 1.0276, 0.7218, 0.9724, 1.2782], q:[0.5, 0.5276], qb:[0.4724, 1.1667], phi:[0.3333]] | [X:[[0]], M:[[1], [-1], [-2], [1], [2]], q:[[0], [-1]], qb:[[1], [0]], phi:[[0]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}M_{1}$, ${ }M_{4}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{5}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }X_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{4}^{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ | ${}$ | -2 | 2*t^2.917 + t^3. + t^3.834 + 2*t^4. + t^4.166 + t^5. + 2*t^5.834 + t^5.917 - 2*t^6. - t^6.083 - t^6.166 + 2*t^6.752 + 2*t^6.917 + t^7.669 + t^7.834 + t^7.917 + 3*t^8. - t^8.083 + t^8.166 + t^8.331 + 2*t^8.752 + t^8.834 - 4*t^8.917 - t^4./y - t^6.917/y + t^7.083/y + t^8.834/y + (2*t^8.917)/y - t^4.*y - t^6.917*y + t^7.083*y + t^8.834*y + 2*t^8.917*y | 2*g1*t^2.917 + t^3. + g1^2*t^3.834 + 2*t^4. + t^4.166/g1^2 + t^5. + 2*g1^2*t^5.834 + g1*t^5.917 - 2*t^6. - t^6.083/g1 - t^6.166/g1^2 + 2*g1^3*t^6.752 + 2*g1*t^6.917 + g1^4*t^7.669 + g1^2*t^7.834 + g1*t^7.917 + 3*t^8. - t^8.083/g1 + t^8.166/g1^2 + t^8.331/g1^4 + 2*g1^3*t^8.752 + g1^2*t^8.834 - 4*g1*t^8.917 - t^4./y - (g1*t^6.917)/y + t^7.083/(g1*y) + (g1^2*t^8.834)/y + (2*g1*t^8.917)/y - t^4.*y - g1*t^6.917*y + (t^7.083*y)/g1 + g1^2*t^8.834*y + 2*g1*t^8.917*y |
Deformation
Here is the data for the deformed fixed points from the chosen fixed point.
# | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from Other Seed Theories
Here is a list of equivalent fixed points from other gauge theories.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from the Same Seed Theory
Below is a list of equivalent fixed points from the same seed theories.
id | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | More Info. | Rational |
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Previous Theory
The previous fixed point before deforming to get the chosen fixed point.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
---|---|---|---|---|---|---|---|---|---|
46446 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{2}M_{4}$ + ${ }q_{2}^{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}^{2}X_{1}$ | 0.5425 | 0.6456 | 0.8403 | [X:[1.3333], M:[0.983, 1.017, 0.7006, 0.983], q:[0.5, 0.517], qb:[0.483, 1.1667], phi:[0.3333]] | t^2.102 + 2*t^2.949 + t^3. + 2*t^4. + t^4.102 + t^4.204 + t^5. + 2*t^5.051 + t^5.102 + 2*t^5.898 + t^5.949 - 2*t^6. - t^4./y - t^4.*y | detail |