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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2266 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{5}q_{1}q_{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}M_{7}$ | 0.6537 | 0.823 | 0.7944 | [M:[1.1706, 0.7314, 0.8294, 0.8294, 0.7314, 0.7804, 1.1706], q:[0.8049, 0.4637], qb:[0.3657, 0.8049], phi:[0.3902]] | [M:[[-6], [-14], [6], [6], [-14], [-4], [-6]], q:[[1], [13]], qb:[[-7], [1]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{2}$, ${ }M_{5}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{4}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{1}$, ${ }M_{7}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{4}M_{5}$, ${ }M_{6}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}M_{6}$, ${ }M_{4}\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{5}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{1}M_{5}$, ${ }M_{2}M_{7}$, ${ }M_{5}M_{7}$, ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}^{3}\tilde{q}_{1}^{2}$, ${ }M_{1}M_{6}$, ${ }M_{6}M_{7}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ | ${}M_{4}M_{7}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$ | -1 | 2*t^2.194 + 2*t^2.341 + t^2.488 + t^3.365 + 2*t^3.512 + t^3.953 + 3*t^4.389 + 4*t^4.536 + 5*t^4.682 + 3*t^4.829 + t^4.976 + 2*t^5.559 + 5*t^5.706 + 3*t^5.853 - t^6. + t^6.294 + t^6.441 + 4*t^6.583 + 7*t^6.73 + 10*t^6.877 + 10*t^7.024 + 3*t^7.171 - t^7.318 - t^7.611 + 3*t^7.754 + 8*t^7.9 + t^7.905 + 7*t^8.047 + t^8.194 - 3*t^8.341 - 5*t^8.488 - t^8.635 + 5*t^8.777 + t^8.782 + 10*t^8.924 + t^8.929 - t^4.171/y - (2*t^6.365)/y - (2*t^6.512)/y + t^7.389/y + (4*t^7.536)/y + (3*t^7.682)/y + (4*t^7.829)/y + (2*t^7.976)/y - t^8.559/y + (2*t^8.706)/y + (2*t^8.853)/y - t^4.171*y - 2*t^6.365*y - 2*t^6.512*y + t^7.389*y + 4*t^7.536*y + 3*t^7.682*y + 4*t^7.829*y + 2*t^7.976*y - t^8.559*y + 2*t^8.706*y + 2*t^8.853*y | (2*t^2.194)/g1^14 + (2*t^2.341)/g1^4 + g1^6*t^2.488 + t^3.365/g1^16 + (2*t^3.512)/g1^6 + g1^24*t^3.953 + (3*t^4.389)/g1^28 + (4*t^4.536)/g1^18 + (5*t^4.682)/g1^8 + 3*g1^2*t^4.829 + g1^12*t^4.976 + (2*t^5.559)/g1^30 + (5*t^5.706)/g1^20 + (3*t^5.853)/g1^10 - t^6. + g1^20*t^6.294 + g1^30*t^6.441 + (4*t^6.583)/g1^42 + (7*t^6.73)/g1^32 + (10*t^6.877)/g1^22 + (10*t^7.024)/g1^12 + (3*t^7.171)/g1^2 - g1^8*t^7.318 - g1^28*t^7.611 + (3*t^7.754)/g1^44 + (8*t^7.9)/g1^34 + g1^48*t^7.905 + (7*t^8.047)/g1^24 + t^8.194/g1^14 - (3*t^8.341)/g1^4 - 5*g1^6*t^8.488 - g1^16*t^8.635 + (5*t^8.777)/g1^56 + g1^26*t^8.782 + (10*t^8.924)/g1^46 + g1^36*t^8.929 - t^4.171/(g1^2*y) - (2*t^6.365)/(g1^16*y) - (2*t^6.512)/(g1^6*y) + t^7.389/(g1^28*y) + (4*t^7.536)/(g1^18*y) + (3*t^7.682)/(g1^8*y) + (4*g1^2*t^7.829)/y + (2*g1^12*t^7.976)/y - t^8.559/(g1^30*y) + (2*t^8.706)/(g1^20*y) + (2*t^8.853)/(g1^10*y) - (t^4.171*y)/g1^2 - (2*t^6.365*y)/g1^16 - (2*t^6.512*y)/g1^6 + (t^7.389*y)/g1^28 + (4*t^7.536*y)/g1^18 + (3*t^7.682*y)/g1^8 + 4*g1^2*t^7.829*y + 2*g1^12*t^7.976*y - (t^8.559*y)/g1^30 + (2*t^8.706*y)/g1^20 + (2*t^8.853*y)/g1^10 |
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 |
---|---|---|---|---|---|---|---|---|---|
1204 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{5}q_{1}q_{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ | 0.6685 | 0.8477 | 0.7886 | [M:[1.1747, 0.7409, 0.8253, 0.8253, 0.7409, 0.7831], q:[0.8042, 0.4549], qb:[0.3704, 0.8042], phi:[0.3916]] | 2*t^2.223 + 2*t^2.349 + 2*t^2.476 + t^3.397 + t^3.524 + t^3.904 + 3*t^4.445 + 4*t^4.572 + 7*t^4.699 + 5*t^4.825 + 3*t^4.952 + 2*t^5.62 + 3*t^5.747 + 2*t^5.873 - t^6. - t^4.175/y - t^4.175*y | detail |