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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57264 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{6}\phi_{1}^{2}$ + ${ }M_{1}M_{7}$ | 0.6434 | 0.7917 | 0.8126 | [M:[0.9565, 1.1652, 1.0841, 0.8348, 0.7478, 1.0841, 1.0435], q:[0.4812, 0.5623], qb:[0.3536, 0.771], phi:[0.458]] | [M:[[-10], [-8], [4], [8], [-12], [4], [10]], q:[[11], [-1]], qb:[[-3], [1]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}M_{5}$, ${ }M_{4}$, ${ }M_{7}$, ${ }M_{3}$, ${ }M_{6}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{5}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{4}M_{5}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{5}M_{6}$, ${ }M_{4}M_{7}$, ${ }M_{2}M_{5}$, ${ }M_{3}M_{4}$, ${ }M_{4}M_{6}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$ | ${}$ | -2 | t^2.243 + t^2.504 + t^3.131 + 2*t^3.252 + t^3.374 + t^3.496 + t^3.878 + t^4. + t^4.122 + t^4.261 + t^4.487 + t^4.504 + 2*t^4.748 + t^5.009 + 2*t^5.496 + t^5.635 + t^5.739 + t^5.757 + t^5.878 - 2*t^6. + t^6.261 + t^6.365 + 2*t^6.383 + 4*t^6.504 + t^6.626 + t^6.73 + t^6.748 + t^6.766 + 2*t^6.991 + t^7.009 + t^7.131 + 3*t^7.252 + t^7.374 + t^7.392 + t^7.496 + 2*t^7.513 + t^7.635 + 2*t^7.739 + t^7.757 + t^7.878 + t^7.982 + 2*t^8. + t^8.122 + 2*t^8.139 - t^8.243 + t^8.261 + t^8.383 - 2*t^8.504 + t^8.522 + t^8.608 + 2*t^8.748 + 2*t^8.766 + t^8.887 + t^8.973 - t^4.374/y - t^6.617/y + t^7.122/y - t^7.626/y + t^7.748/y + t^8.131/y + t^8.374/y + (2*t^8.496)/y + t^8.617/y + t^8.635/y + t^8.739/y + (2*t^8.757)/y - t^8.861/y + t^8.878/y - t^4.374*y - t^6.617*y + t^7.122*y - t^7.626*y + t^7.748*y + t^8.131*y + t^8.374*y + 2*t^8.496*y + t^8.617*y + t^8.635*y + t^8.739*y + 2*t^8.757*y - t^8.861*y + t^8.878*y | t^2.243/g1^12 + g1^8*t^2.504 + g1^10*t^3.131 + 2*g1^4*t^3.252 + t^3.374/g1^2 + t^3.496/g1^8 + g1^6*t^3.878 + t^4. + t^4.122/g1^6 + g1^20*t^4.261 + t^4.487/g1^24 + g1^8*t^4.504 + (2*t^4.748)/g1^4 + g1^16*t^5.009 + (2*t^5.496)/g1^8 + g1^18*t^5.635 + t^5.739/g1^20 + g1^12*t^5.757 + g1^6*t^5.878 - 2*t^6. + g1^20*t^6.261 + t^6.365/g1^18 + 2*g1^14*t^6.383 + 4*g1^8*t^6.504 + g1^2*t^6.626 + t^6.73/g1^36 + t^6.748/g1^4 + g1^28*t^6.766 + (2*t^6.991)/g1^16 + g1^16*t^7.009 + g1^10*t^7.131 + 3*g1^4*t^7.252 + t^7.374/g1^2 + g1^30*t^7.392 + t^7.496/g1^8 + 2*g1^24*t^7.513 + g1^18*t^7.635 + (2*t^7.739)/g1^20 + g1^12*t^7.757 + g1^6*t^7.878 + t^7.982/g1^32 + 2*t^8. + t^8.122/g1^6 + 2*g1^26*t^8.139 - t^8.243/g1^12 + g1^20*t^8.261 + g1^14*t^8.383 - 2*g1^8*t^8.504 + g1^40*t^8.522 + t^8.608/g1^30 + (2*t^8.748)/g1^4 + 2*g1^28*t^8.766 + g1^22*t^8.887 + t^8.973/g1^48 - t^4.374/(g1^2*y) - t^6.617/(g1^14*y) + t^7.122/(g1^6*y) - (g1^2*t^7.626)/y + t^7.748/(g1^4*y) + (g1^10*t^8.131)/y + t^8.374/(g1^2*y) + (2*t^8.496)/(g1^8*y) + t^8.617/(g1^14*y) + (g1^18*t^8.635)/y + t^8.739/(g1^20*y) + (2*g1^12*t^8.757)/y - t^8.861/(g1^26*y) + (g1^6*t^8.878)/y - (t^4.374*y)/g1^2 - (t^6.617*y)/g1^14 + (t^7.122*y)/g1^6 - g1^2*t^7.626*y + (t^7.748*y)/g1^4 + g1^10*t^8.131*y + (t^8.374*y)/g1^2 + (2*t^8.496*y)/g1^8 + (t^8.617*y)/g1^14 + g1^18*t^8.635*y + (t^8.739*y)/g1^20 + 2*g1^12*t^8.757*y - (t^8.861*y)/g1^26 + g1^6*t^8.878*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 |
---|---|---|---|---|---|---|---|---|---|
55617 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{6}\phi_{1}^{2}$ | 0.6488 | 0.8006 | 0.8104 | [M:[0.9267, 1.1413, 1.096, 0.8587, 0.712, 1.096], q:[0.514, 0.5593], qb:[0.3447, 0.774], phi:[0.452]] | t^2.136 + t^2.576 + t^2.78 + 2*t^3.288 + t^3.356 + t^3.424 + t^3.932 + t^4. + t^4.068 + t^4.272 + t^4.44 + t^4.576 + 2*t^4.712 + t^4.916 + t^5.152 + 2*t^5.424 + 2*t^5.56 + t^5.864 + t^5.932 - 2*t^6. - t^4.356/y - t^4.356*y | detail |