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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1120 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}q_{1}q_{2}$ + ${ }M_{6}q_{1}\tilde{q}_{1}$ | 0.6838 | 0.8483 | 0.8061 | [M:[1.0879, 1.0879, 1.0167, 0.9121, 0.8076, 0.7364], q:[0.772, 0.4205], qb:[0.4916, 0.4916], phi:[0.4561]] | [M:[[4], [4], [-22], [-4], [14], [-12]], q:[[1], [-15]], qb:[[11], [11]], phi:[[-2]]] | 1 | {a: 144062/210681, c: 357433/421362, M1: 1498/1377, M2: 1498/1377, M3: 1400/1377, M4: 1256/1377, M5: 1112/1377, M6: 338/459, q1: 1063/1377, q2: 193/459, qb1: 677/1377, qb2: 677/1377, phi1: 628/1377} |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}M_{6}$, ${ }M_{5}$, ${ }M_{4}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }M_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{6}^{2}$, ${ }M_{5}M_{6}$, ${ }M_{5}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{4}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{1}M_{6}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{1}M_{5}$ | ${}M_{1}\phi_{1}^{2}$, ${ }M_{6}q_{1}\tilde{q}_{2}$ | -2 | t^2.209 + t^2.423 + 2*t^2.736 + t^3.05 + t^3.264 + t^3.791 + t^3.891 + 2*t^4.105 + 3*t^4.318 + t^4.418 + t^4.632 + t^4.845 + 2*t^4.946 + 2*t^5.159 + t^5.259 + 5*t^5.473 + t^5.686 - 2*t^6. + 2*t^6.1 - t^6.214 + 3*t^6.314 + 5*t^6.527 + 3*t^6.627 + 3*t^6.741 + 3*t^6.841 + t^6.941 + 5*t^7.054 + 2*t^7.155 + t^7.268 + t^7.368 + t^7.468 + t^7.582 + 4*t^7.682 + t^7.782 + 3*t^7.895 + 2*t^7.996 + 2*t^8.109 + 4*t^8.209 + 2*t^8.309 - 2*t^8.423 + 3*t^8.523 + 4*t^8.636 - t^8.736 + 3*t^8.837 + t^8.95 - t^4.368/y - t^6.577/y - t^6.791/y + t^7.318/y - t^7.418/y + t^7.632/y + (3*t^7.946)/y + (3*t^8.159)/y + t^8.259/y + (3*t^8.473)/y + t^8.686/y + t^8.786/y - t^4.368*y - t^6.577*y - t^6.791*y + t^7.318*y - t^7.418*y + t^7.632*y + 3*t^7.946*y + 3*t^8.159*y + t^8.259*y + 3*t^8.473*y + t^8.686*y + t^8.786*y | t^2.209/g1^12 + g1^14*t^2.423 + (2*t^2.736)/g1^4 + t^3.05/g1^22 + g1^4*t^3.264 + g1^12*t^3.791 + t^3.891/g1^32 + (2*t^4.105)/g1^6 + 3*g1^20*t^4.318 + t^4.418/g1^24 + g1^2*t^4.632 + g1^28*t^4.845 + (2*t^4.946)/g1^16 + 2*g1^10*t^5.159 + t^5.259/g1^34 + (5*t^5.473)/g1^8 + g1^18*t^5.686 - 2*t^6. + (2*t^6.1)/g1^44 - g1^26*t^6.214 + (3*t^6.314)/g1^18 + 5*g1^8*t^6.527 + (3*t^6.627)/g1^36 + 3*g1^34*t^6.741 + (3*t^6.841)/g1^10 + t^6.941/g1^54 + 5*g1^16*t^7.054 + (2*t^7.155)/g1^28 + g1^42*t^7.268 + t^7.368/g1^2 + t^7.468/g1^46 + g1^24*t^7.582 + (4*t^7.682)/g1^20 + t^7.782/g1^64 + 3*g1^6*t^7.895 + (2*t^7.996)/g1^38 + 2*g1^32*t^8.109 + (4*t^8.209)/g1^12 + (2*t^8.309)/g1^56 - 2*g1^14*t^8.423 + (3*t^8.523)/g1^30 + 4*g1^40*t^8.636 - t^8.736/g1^4 + (3*t^8.837)/g1^48 + g1^22*t^8.95 - t^4.368/(g1^2*y) - t^6.577/(g1^14*y) - (g1^12*t^6.791)/y + (g1^20*t^7.318)/y - t^7.418/(g1^24*y) + (g1^2*t^7.632)/y + (3*t^7.946)/(g1^16*y) + (3*g1^10*t^8.159)/y + t^8.259/(g1^34*y) + (3*t^8.473)/(g1^8*y) + (g1^18*t^8.686)/y + t^8.786/(g1^26*y) - (t^4.368*y)/g1^2 - (t^6.577*y)/g1^14 - g1^12*t^6.791*y + g1^20*t^7.318*y - (t^7.418*y)/g1^24 + g1^2*t^7.632*y + (3*t^7.946*y)/g1^16 + 3*g1^10*t^8.159*y + (t^8.259*y)/g1^34 + (3*t^8.473*y)/g1^8 + g1^18*t^8.686*y + (t^8.786*y)/g1^26 |
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 |
---|---|---|---|---|---|---|---|---|---|
694 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}q_{1}q_{2}$ | 0.6643 | 0.8125 | 0.8176 | [M:[1.086, 1.086, 1.0269, 0.914, 0.8011], q:[0.7715, 0.4274], qb:[0.4866, 0.4866], phi:[0.457]] | t^2.403 + 2*t^2.742 + t^3.081 + t^3.258 + 2*t^3.774 + t^3.935 + 2*t^4.113 + 3*t^4.29 + t^4.806 + 2*t^5.145 + 4*t^5.484 + t^5.661 - 3*t^6. - t^4.371/y - t^4.371*y | detail |