Resistance 3: Y114.14 (March 7 high) Resistance 2: Y113.48 (March 17 high) Resistance 1: Y112.86 (March 21 high) Current price: Y111.80 Support 1: Y110.
Resistance 3: Chf1.0137 (March 10 high) Resistance 2: Chf1.0103 (March 15 high) Resistance 1: Chf1.0043 (February 20 high) Current price: Chf1.0012 Support 1: Chf0.
Resistance 3: $ 1.2637 (January 25 high) Resistance 2: $ 1.2595 (March 28 high) Resistance 1: $ 1.2530 (March 23 high) Current price: $ 1.2450 Support 1: $ 1.
Resistance 3: $ 1.0872 (March 28 high) Resistance 2: $ 1.0826 (March 29 high) Resistance 1: $ 1.0769 (March 30 high) Current price: $ 1.0678 Support 1: $ 1.
Resistance 3: $ 1283-91 (Nov 10 highs) Resistance 2: $ 1257-60 (Mar 27-28 highs) Resistance 1: $ 1250 (high of the US session on Mar 30) Current price: $ 1241 Support 1: $ 1239 (high of t.
Resistance 3: Y113.45-55 (Mar 16-17 highs) Resistance 2: Y112.85 (Mar 20 high) Resistance 1: Y112.20-25 (highs of the US session on Mar 21) Current price: Y112.09 Support 1: Y111.
Resistance 3: ₣ 1.0105-15 (Mar 13-14 highs) Resistance 2: ₣ 1.0060-65 (Mar 13 lows) Resistance 1: ₣ 1.0010 (Mar 30 high) Current price: ₣ 1.0010 Support 1: ₣ 0.
Resistance 3: $ 1.2655 (Feb 1 high) Resistance 2: $ 1.2595-15 (Mar 27-28 highs) Resistance 1: $ 1.2520-35 (high of the US session on Mar 28 and Mar 30 high) Current price: $ 1.
Resistance 3: $ 1.0825 (Mar 29 high) Resistance 2: $ 1.0795 (high of the US session on Mar 29, MA 200 H1) Resistance 1: $ 1.0750 (high of the US session on Mar 30) Current price: $ 1.
Resistance 3: C $ 1.3410 (Mar 28 high) Resistance 2: C $ 1.3385 (Mar 24 high) Resistance 1: C $ 1.3350 (Mar 28 low, MA (200) H1) Current price: C $ 1.3344 Support 1: C $ 1.
Resistance 3: $ 0.7070 (Mar 27 high) Resistance 2: $ 0.7030 / 45 (Mar 29 high, MA (200) H1) Resistance 1: $ 0.7015 (Mar 22 low) Current price: $ 0.6992 Support 2: $ 0.
Resistance 3: $ 0.7750 (Mar 21 high) Resistance 2: $ 0.7720 (Mar 15 high) Resistance 1: $ 0.7680 (Mar 30 high) Current price: $ 0.7664 Support 1: $ 0.7630 (Mar 29 low) Support 2: $ 0.
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