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 |
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79542 | Sp2s2nf1 | ${}M_{1}S_{1}S_{2}$ + ${ }M_{2}S_{1}^{2}$ + ${ }M_{2}^{2}$ + ${ }q_{2}^{2}S_{1}$ | 2.3559 | 2.4523 | 0.9607 | [X:[], M:[0.8972, 1.0], q:[0.6329, 0.75], qb:[], phi:[], S:[0.5, 0.6028], Sb:[], A:[], Ab:[]] | [X:[], M:[[-1], [0]], q:[[-6], [0]], qb:[], phi:[], S:[[0], [1]], Sb:[], A:[], Ab:[]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{1}$, ${ }M_{2}$, ${ }S_{2}^{2}$, ${ }q_{1}q_{2}$, ${ }q_{1}^{2}S_{1}$, ${ }M_{1}^{2}$, ${ }q_{1}^{2}S_{2}$, ${ }q_{1}q_{2}S_{2}$ | ${}S_{1}^{4}$ | 0 | t^2.691 + t^3. + t^3.617 + t^4.149 + t^5.298 + t^5.383 + t^5.606 + t^5.957 + 2*t^6.309 - t^6.351 + 3*t^6.617 + t^6.84 + t^6.926 + t^7.106 + t^7.149 + 2*t^7.234 + t^7.457 - t^7.5 + 2*t^7.766 - t^7.809 + t^8.074 - t^8.16 + t^8.202 + 3*t^8.298 - t^8.34 + 3*t^8.606 - 2*t^8.691 + 3*t^8.915 + 2*t^8.957 - t^4.5/y - t^4.809/y - (2*t^7.5)/y - (2*t^7.809)/y - (2*t^8.117)/y - (2*t^8.426)/y - t^8.649/y + t^8.691/y - t^8.957/y - t^4.5*y - t^4.809*y - 2*t^7.5*y - 2*t^7.809*y - 2*t^8.117*y - 2*t^8.426*y - t^8.649*y + t^8.691*y - t^8.957*y | t^2.691/g1 + t^3. + g1^2*t^3.617 + t^4.149/g1^6 + t^5.298/g1^12 + t^5.383/g1^2 + t^5.606/g1^11 + t^5.957/g1^5 + 2*g1*t^6.309 - g1^6*t^6.351 + 3*g1^2*t^6.617 + t^6.84/g1^7 + g1^3*t^6.926 + t^7.106/g1^11 + t^7.149/g1^6 + 2*g1^4*t^7.234 + t^7.457/g1^5 - t^7.5 + (2*t^7.766)/g1^4 - g1*t^7.809 + t^8.074/g1^3 - g1^7*t^8.16 + g1^12*t^8.202 + (3*t^8.298)/g1^12 - t^8.34/g1^7 + (3*t^8.606)/g1^11 - (2*t^8.691)/g1 + (3*t^8.915)/g1^10 + (2*t^8.957)/g1^5 - t^4.5/y - (g1*t^4.809)/y - (2*t^7.5)/y - (2*g1*t^7.809)/y - (2*g1^2*t^8.117)/y - (2*g1^3*t^8.426)/y - t^8.649/(g1^6*y) + t^8.691/(g1*y) - t^8.957/(g1^5*y) - t^4.5*y - g1*t^4.809*y - 2*t^7.5*y - 2*g1*t^7.809*y - 2*g1^2*t^8.117*y - 2*g1^3*t^8.426*y - (t^8.649*y)/g1^6 + (t^8.691*y)/g1 - (t^8.957*y)/g1^5 |
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 |
---|---|---|---|---|---|---|---|---|---|
79513 | Sp2s2nf1 | ${}M_{1}S_{1}S_{2}$ + ${ }M_{2}S_{1}^{2}$ + ${ }M_{2}^{2}$ | 2.3699 | 2.4822 | 0.9548 | [X:[], M:[0.8802, 1.0], q:[0.6407, 0.6407], qb:[], phi:[], S:[0.5, 0.6198], Sb:[], A:[], Ab:[]] | t^2.641 + t^3. + t^3.719 + t^3.844 + t^5.281 + 3*t^5.344 + 3*t^5.704 - 3*t^6. - t^4.5/y - t^4.859/y - t^4.5*y - t^4.859*y | detail |