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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56305 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}\phi_{1}^{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{6}$ + ${ }M_{5}^{2}$ + ${ }M_{7}\tilde{q}_{1}\tilde{q}_{2}$ | 0.7078 | 0.8734 | 0.8103 | [M:[1.067, 0.8995, 0.933, 1.0335, 1.0, 0.9665, 0.866], q:[0.5168, 0.4162], qb:[0.5838, 0.5503], phi:[0.4832]] | [M:[[4], [-6], [-4], [2], [0], [-2], [-8]], q:[[1], [-5]], qb:[[5], [3]], phi:[[-1]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{7}$, ${ }M_{2}$, ${ }M_{3}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{5}$, ${ }M_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{7}^{2}$, ${ }M_{2}M_{7}$, ${ }M_{2}^{2}$, ${ }M_{3}M_{7}$, ${ }M_{2}M_{3}$, ${ }M_{6}M_{7}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{3}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{5}M_{7}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{2}M_{5}$, ${ }M_{3}M_{6}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{6}^{2}$, ${ }M_{1}M_{7}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{1}M_{2}$, ${ }M_{5}M_{6}$, ${ }M_{5}\phi_{1}^{2}$ | ${}$ | -2 | t^2.598 + t^2.698 + t^2.799 + 2*t^2.899 + t^3. + t^3.201 + t^3.947 + t^4.249 + t^4.349 + t^4.45 + t^4.55 + t^4.651 + 2*t^4.751 + t^4.852 + t^4.952 + t^5.196 + t^5.296 + 2*t^5.397 + 2*t^5.497 + 3*t^5.598 + 2*t^5.698 + 4*t^5.799 + t^5.899 - 2*t^6. - t^6.201 - t^6.302 - t^6.503 + t^6.545 + t^6.646 + t^6.746 + 3*t^6.847 + 2*t^6.947 + t^7.048 + 4*t^7.148 + 4*t^7.249 + 3*t^7.349 + 3*t^7.45 + 3*t^7.55 + 3*t^7.651 + 2*t^7.751 + t^7.794 + 2*t^7.894 + 2*t^7.995 - t^8.053 + 3*t^8.095 + 4*t^8.196 + 4*t^8.296 + 5*t^8.397 + 4*t^8.497 + t^8.598 + 3*t^8.698 - 2*t^8.799 - 6*t^8.899 - t^4.45/y - t^7.048/y - t^7.148/y - t^7.349/y + t^7.55/y + t^7.751/y + t^7.852/y + t^8.296/y + t^8.397/y + (3*t^8.497)/y + (3*t^8.598)/y + (3*t^8.698)/y + (3*t^8.799)/y + (3*t^8.899)/y - t^4.45*y - t^7.048*y - t^7.148*y - t^7.349*y + t^7.55*y + t^7.751*y + t^7.852*y + t^8.296*y + t^8.397*y + 3*t^8.497*y + 3*t^8.598*y + 3*t^8.698*y + 3*t^8.799*y + 3*t^8.899*y | t^2.598/g1^8 + t^2.698/g1^6 + t^2.799/g1^4 + (2*t^2.899)/g1^2 + t^3. + g1^4*t^3.201 + t^3.947/g1^11 + t^4.249/g1^5 + t^4.349/g1^3 + t^4.45/g1 + g1*t^4.55 + g1^3*t^4.651 + 2*g1^5*t^4.751 + g1^7*t^4.852 + g1^9*t^4.952 + t^5.196/g1^16 + t^5.296/g1^14 + (2*t^5.397)/g1^12 + (2*t^5.497)/g1^10 + (3*t^5.598)/g1^8 + (2*t^5.698)/g1^6 + (4*t^5.799)/g1^4 + t^5.899/g1^2 - 2*t^6. - g1^4*t^6.201 - g1^6*t^6.302 - g1^10*t^6.503 + t^6.545/g1^19 + t^6.646/g1^17 + t^6.746/g1^15 + (3*t^6.847)/g1^13 + (2*t^6.947)/g1^11 + t^7.048/g1^9 + (4*t^7.148)/g1^7 + (4*t^7.249)/g1^5 + (3*t^7.349)/g1^3 + (3*t^7.45)/g1 + 3*g1*t^7.55 + 3*g1^3*t^7.651 + 2*g1^5*t^7.751 + t^7.794/g1^24 + (2*t^7.894)/g1^22 + (2*t^7.995)/g1^20 - g1^11*t^8.053 + (3*t^8.095)/g1^18 + (4*t^8.196)/g1^16 + (4*t^8.296)/g1^14 + (5*t^8.397)/g1^12 + (4*t^8.497)/g1^10 + t^8.598/g1^8 + (3*t^8.698)/g1^6 - (2*t^8.799)/g1^4 - (6*t^8.899)/g1^2 - t^4.45/(g1*y) - t^7.048/(g1^9*y) - t^7.148/(g1^7*y) - t^7.349/(g1^3*y) + (g1*t^7.55)/y + (g1^5*t^7.751)/y + (g1^7*t^7.852)/y + t^8.296/(g1^14*y) + t^8.397/(g1^12*y) + (3*t^8.497)/(g1^10*y) + (3*t^8.598)/(g1^8*y) + (3*t^8.698)/(g1^6*y) + (3*t^8.799)/(g1^4*y) + (3*t^8.899)/(g1^2*y) - (t^4.45*y)/g1 - (t^7.048*y)/g1^9 - (t^7.148*y)/g1^7 - (t^7.349*y)/g1^3 + g1*t^7.55*y + g1^5*t^7.751*y + g1^7*t^7.852*y + (t^8.296*y)/g1^14 + (t^8.397*y)/g1^12 + (3*t^8.497*y)/g1^10 + (3*t^8.598*y)/g1^8 + (3*t^8.698*y)/g1^6 + (3*t^8.799*y)/g1^4 + (3*t^8.899*y)/g1^2 |
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 |
---|---|---|---|---|---|---|---|---|---|
51774 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}\phi_{1}^{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{6}$ + ${ }M_{5}^{2}$ | 0.6977 | 0.8546 | 0.8164 | [M:[1.0436, 0.9346, 0.9564, 1.0218, 1.0, 0.9782], q:[0.5109, 0.4455], qb:[0.5545, 0.5327], phi:[0.4891]] | t^2.804 + t^2.869 + 2*t^2.935 + t^3. + t^3.131 + t^3.262 + t^4.14 + t^4.336 + t^4.402 + t^4.467 + t^4.533 + t^4.598 + 2*t^4.664 + t^4.729 + t^4.795 + t^5.607 + 2*t^5.738 + 2*t^5.804 + 3*t^5.869 + t^5.935 - 2*t^6. - t^4.467/y - t^4.467*y | detail |