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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58798 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{6}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{7}\phi_{1}^{2}$ + ${ }M_{1}M_{8}$ | 0.686 | 0.8619 | 0.7959 | [M:[1.185, 0.9649, 0.815, 0.815, 0.9649, 0.74, 1.11, 0.815], q:[0.4075, 0.4075], qb:[0.6276, 0.7775], phi:[0.445]] | [M:[[2], [-22], [-2], [-2], [-22], [8], [12], [-2]], q:[[-1], [-1]], qb:[[23], [3]], phi:[[-6]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}M_{6}$, ${ }M_{3}$, ${ }M_{4}$, ${ }M_{8}$, ${ }M_{2}$, ${ }M_{5}$, ${ }M_{7}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{6}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{3}M_{6}$, ${ }M_{4}M_{6}$, ${ }M_{6}M_{8}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}^{2}$, ${ }M_{3}M_{8}$, ${ }M_{4}M_{8}$, ${ }M_{8}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{4}$, ${ }M_{3}M_{5}$, ${ }M_{4}M_{5}$, ${ }M_{2}M_{8}$, ${ }M_{5}M_{8}$, ${ }M_{6}M_{7}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}M_{7}$, ${ }M_{4}M_{7}$, ${ }M_{7}M_{8}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{5}$, ${ }M_{5}^{2}$ | ${}M_{6}\phi_{1}q_{1}^{2}$, ${ }M_{6}\phi_{1}q_{2}^{2}$ | -3 | t^2.22 + 3*t^2.445 + 2*t^2.895 + t^3.33 + 2*t^3.78 + t^4.215 + 3*t^4.44 + 3*t^4.665 + 6*t^4.89 + t^5.1 + 2*t^5.115 + 4*t^5.34 + t^5.55 + 3*t^5.775 + 3*t^5.789 - 3*t^6. + 6*t^6.225 + t^6.435 - t^6.45 + 4*t^6.66 + 2*t^6.675 + 6*t^6.885 + 5*t^7.11 + t^7.321 + 10*t^7.335 + 3*t^7.545 + 6*t^7.56 + t^7.77 + 6*t^7.785 + t^7.995 + 3*t^8.01 + 3*t^8.22 + 6*t^8.234 + t^8.431 - 9*t^8.445 + t^8.656 + 9*t^8.67 + 4*t^8.684 + 5*t^8.88 - 8*t^8.895 - t^4.335/y - t^6.555/y - (2*t^6.78)/y - (2*t^7.23)/y + (2*t^7.44)/y + (3*t^7.665)/y + (5*t^7.89)/y + (3*t^8.115)/y + (6*t^8.34)/y + t^8.55/y + (2*t^8.775)/y + t^8.789/y - t^4.335*y - t^6.555*y - 2*t^6.78*y - 2*t^7.23*y + 2*t^7.44*y + 3*t^7.665*y + 5*t^7.89*y + 3*t^8.115*y + 6*t^8.34*y + t^8.55*y + 2*t^8.775*y + t^8.789*y | g1^8*t^2.22 + (3*t^2.445)/g1^2 + (2*t^2.895)/g1^22 + g1^12*t^3.33 + (2*t^3.78)/g1^8 + g1^26*t^4.215 + 3*g1^16*t^4.44 + 3*g1^6*t^4.665 + (6*t^4.89)/g1^4 + g1^40*t^5.1 + (2*t^5.115)/g1^14 + (4*t^5.34)/g1^24 + g1^20*t^5.55 + 3*g1^10*t^5.775 + (3*t^5.789)/g1^44 - 3*t^6. + (6*t^6.225)/g1^10 + g1^34*t^6.435 - t^6.45/g1^20 + 4*g1^24*t^6.66 + (2*t^6.675)/g1^30 + 6*g1^14*t^6.885 + 5*g1^4*t^7.11 + g1^48*t^7.321 + (10*t^7.335)/g1^6 + 3*g1^38*t^7.545 + (6*t^7.56)/g1^16 + g1^28*t^7.77 + (6*t^7.785)/g1^26 + g1^18*t^7.995 + (3*t^8.01)/g1^36 + 3*g1^8*t^8.22 + (6*t^8.234)/g1^46 + g1^52*t^8.431 - (9*t^8.445)/g1^2 + g1^42*t^8.656 + (9*t^8.67)/g1^12 + (4*t^8.684)/g1^66 + 5*g1^32*t^8.88 - (8*t^8.895)/g1^22 - t^4.335/(g1^6*y) - (g1^2*t^6.555)/y - (2*t^6.78)/(g1^8*y) - (2*t^7.23)/(g1^28*y) + (2*g1^16*t^7.44)/y + (3*g1^6*t^7.665)/y + (5*t^7.89)/(g1^4*y) + (3*t^8.115)/(g1^14*y) + (6*t^8.34)/(g1^24*y) + (g1^20*t^8.55)/y + (2*g1^10*t^8.775)/y + t^8.789/(g1^44*y) - (t^4.335*y)/g1^6 - g1^2*t^6.555*y - (2*t^6.78*y)/g1^8 - (2*t^7.23*y)/g1^28 + 2*g1^16*t^7.44*y + 3*g1^6*t^7.665*y + (5*t^7.89*y)/g1^4 + (3*t^8.115*y)/g1^14 + (6*t^8.34*y)/g1^24 + g1^20*t^8.55*y + 2*g1^10*t^8.775*y + (t^8.789*y)/g1^44 |
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 |
---|---|---|---|---|---|---|---|---|---|
56676 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{6}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{7}\phi_{1}^{2}$ | 0.6704 | 0.8348 | 0.8031 | [M:[1.1847, 0.9683, 0.8153, 0.8153, 0.9683, 0.7388, 1.1082], q:[0.4077, 0.4077], qb:[0.624, 0.777], phi:[0.4459]] | t^2.216 + 2*t^2.446 + 2*t^2.905 + t^3.325 + t^3.554 + 2*t^3.784 + t^4.203 + 3*t^4.433 + 2*t^4.662 + 3*t^4.892 + t^5.082 + 2*t^5.121 + 2*t^5.351 + t^5.541 + 3*t^5.77 + 3*t^5.81 - t^6. - t^4.338/y - t^4.338*y | detail |