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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57060 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{3}M_{4}$ + ${ }\phi_{1}q_{1}q_{2}$ + ${ }M_{1}X_{1}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{3}M_{6}$ + ${ }M_{2}M_{5}$ + ${ }M_{7}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ | 0.596 | 0.7558 | 0.7886 | [X:[1.5739], M:[0.4261, 0.9827, 1.2783, 0.7217, 1.0173, 0.7217, 0.8522], q:[0.6392, 0.9347], qb:[0.3781, 0.3436], phi:[0.4261]] | [X:[[2]], M:[[-2], [-14], [-6], [6], [14], [6], [-4]], q:[[-3], [5]], qb:[[17], [-11]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}M_{4}$, ${ }M_{6}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }M_{2}$, ${ }M_{5}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{6}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{4}M_{7}$, ${ }M_{6}M_{7}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }X_{1}$, ${ }M_{2}M_{4}$, ${ }M_{2}M_{6}$, ${ }M_{7}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{4}M_{5}$, ${ }M_{5}M_{6}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{2}M_{7}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{6}\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{5}M_{7}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}^{2}$, ${ }M_{7}\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}\tilde{q}_{2}^{2}$ | ${}$ | -2 | 2*t^2.165 + 2*t^2.557 + t^2.948 + t^3.052 + t^3.34 + t^3.547 + t^3.938 + 3*t^4.33 + 5*t^4.722 + 5*t^5.113 + 2*t^5.217 + 3*t^5.505 + t^5.608 + 2*t^5.712 + 2*t^5.896 - 2*t^6. + 4*t^6.104 + t^6.288 - t^6.392 + 5*t^6.495 + t^6.599 + t^6.68 - 2*t^6.783 + 6*t^6.887 + t^7.094 - t^7.175 + 9*t^7.278 + t^7.382 + t^7.485 + 8*t^7.67 + t^7.773 + 4*t^7.877 + 5*t^8.062 - 5*t^8.165 + 7*t^8.269 + 4*t^8.453 - 8*t^8.557 + 9*t^8.66 + 2*t^8.764 + 3*t^8.845 - 8*t^8.948 - t^4.278/y - t^6.443/y - (2*t^6.835)/y + t^7.33/y + (6*t^7.722)/y + (4*t^8.113)/y + (2*t^8.217)/y + (4*t^8.505)/y + t^8.608/y + (2*t^8.712)/y + (2*t^8.896)/y - t^4.278*y - t^6.443*y - 2*t^6.835*y + t^7.33*y + 6*t^7.722*y + 4*t^8.113*y + 2*t^8.217*y + 4*t^8.505*y + t^8.608*y + 2*t^8.712*y + 2*t^8.896*y | 2*g1^6*t^2.165 + (2*t^2.557)/g1^4 + t^2.948/g1^14 + g1^14*t^3.052 + t^3.34/g1^24 + g1^32*t^3.547 + g1^22*t^3.938 + 3*g1^12*t^4.33 + 5*g1^2*t^4.722 + (5*t^5.113)/g1^8 + 2*g1^20*t^5.217 + (3*t^5.505)/g1^18 + g1^10*t^5.608 + 2*g1^38*t^5.712 + (2*t^5.896)/g1^28 - 2*t^6. + 4*g1^28*t^6.104 + t^6.288/g1^38 - t^6.392/g1^10 + 5*g1^18*t^6.495 + g1^46*t^6.599 + t^6.68/g1^48 - (2*t^6.783)/g1^20 + 6*g1^8*t^6.887 + g1^64*t^7.094 - t^7.175/g1^30 + (9*t^7.278)/g1^2 + g1^26*t^7.382 + g1^54*t^7.485 + (8*t^7.67)/g1^12 + g1^16*t^7.773 + 4*g1^44*t^7.877 + (5*t^8.062)/g1^22 - 5*g1^6*t^8.165 + 7*g1^34*t^8.269 + (4*t^8.453)/g1^32 - (8*t^8.557)/g1^4 + 9*g1^24*t^8.66 + 2*g1^52*t^8.764 + (3*t^8.845)/g1^42 - (8*t^8.948)/g1^14 - t^4.278/(g1^2*y) - (g1^4*t^6.443)/y - (2*t^6.835)/(g1^6*y) + (g1^12*t^7.33)/y + (6*g1^2*t^7.722)/y + (4*t^8.113)/(g1^8*y) + (2*g1^20*t^8.217)/y + (4*t^8.505)/(g1^18*y) + (g1^10*t^8.608)/y + (2*g1^38*t^8.712)/y + (2*t^8.896)/(g1^28*y) - (t^4.278*y)/g1^2 - g1^4*t^6.443*y - (2*t^6.835*y)/g1^6 + g1^12*t^7.33*y + 6*g1^2*t^7.722*y + (4*t^8.113*y)/g1^8 + 2*g1^20*t^8.217*y + (4*t^8.505*y)/g1^18 + g1^10*t^8.608*y + 2*g1^38*t^8.712*y + (2*t^8.896*y)/g1^28 |
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 |
---|---|---|---|---|---|---|---|---|---|
55459 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{3}M_{4}$ + ${ }\phi_{1}q_{1}q_{2}$ + ${ }M_{1}X_{1}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{3}M_{6}$ + ${ }M_{2}M_{5}$ | 0.5831 | 0.734 | 0.7944 | [X:[1.5732], M:[0.4268, 0.9873, 1.2803, 0.7197, 1.0127, 0.7197], q:[0.6401, 0.9331], qb:[0.3725, 0.3472], phi:[0.4268]] | 2*t^2.159 + t^2.561 + t^2.962 + t^3.038 + t^3.363 + t^3.439 + t^3.516 + t^3.917 + 3*t^4.318 + 3*t^4.72 + 3*t^5.121 + 2*t^5.197 + 2*t^5.523 + 2*t^5.599 + 2*t^5.675 + t^5.924 - t^6. - t^4.28/y - t^4.28*y | detail |